ScalingStacks

3.1.5. Differential

Let Hnil​(W)=𝐅2βŠ—H𝐙nil​(W)H^{\mathrm{nil}}(W)={\mathbf{F}}_{2}\otimes H_{\mathbf{Z}}^{\mathrm{nil}}(W). We define a linear map d:Hnil​(W)β†’Hnil​(W)d:H^{\mathrm{nil}}(W)\to H^{\mathrm{nil}}(W) by

d⁑(Tw)=βˆ‘wβ€²<w,ℓ⁑(wβ€²)=ℓ⁑(w)βˆ’1Twβ€².d(T_{w})=\sum_{w^{\prime}<w,\ \ell(w^{\prime})=\ell(w)-1}T_{w^{\prime}}.
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Proposition 3.1.3. The map dd defines a structure of differential graded algebra on Hnil​(W)H^{\mathrm{nil}}(W).

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Proof. Let w∈Ww\in W and s∈Ss\in S with w​s>wws>w. We have d⁑(Tw​Ts)=d⁑(Tw​s)=βˆ‘wβ€²<w​s,ℓ⁑(wβ€²)=ℓ⁑(w)Twβ€²d(T_{w}T_{s})=d(T_{ws})=\sum_{w^{\prime}<ws,\ \ell(w^{\prime})=\ell(w)}T_{w^{\prime}}. We have [Hu, Theorem 5.10]

{wβ€²βˆˆW|wβ€²<ws,β„“(wβ€²)=β„“(w)}={wβ€²β€²s|wβ€²β€²<w,wβ€²β€²<wβ€²β€²s,β„“(wβ€²β€²)=β„“(w)βˆ’1}βŠ”{w}.\{w^{\prime}\in W\ |w^{\prime}<ws,\ \ell(w^{\prime})=\ell(w)\}=\{w^{\prime\prime}s\ |\ w^{\prime\prime}<w,\ w^{\prime\prime}<w^{\prime\prime}s,\ \ell(w^{\prime\prime})=\ell(w)-1\}\sqcup\{w\}.

It follows that d⁑(Tw​Ts)=d⁑(Tw)​Ts+Tw=d⁑(Tw)​Ts+Tw​d​(Ts)d(T_{w}T_{s})=d(T_{w})T_{s}+T_{w}=d(T_{w})T_{s}+T_{w}d(T_{s}).

Consider now v∈Wv\in W and s∈Ss\in S with v​s<vvs<v. We have d⁑(Tv)=d⁑(Tv​s​Ts)=d⁑(Tv​s)​Ts+Tv​sd(T_{v})=d(T_{vs}T_{s})=d(T_{vs})T_{s}+T_{vs} by the result above. It follows that d⁑(Tv)​Ts+Tv​d​(Ts)=Tv​s​Ts+Tv=0=d⁑(Tv​Ts)d(T_{v})T_{s}+T_{v}d(T_{s})=T_{vs}T_{s}+T_{v}=0=d(T_{v}T_{s}).

We deduce that d⁑(Tw​Twβ€²)=d⁑(Tw)​Twβ€²+Tw​d​(Twβ€²)d(T_{w}T_{w^{\prime}})=d(T_{w})T_{w^{\prime}}+T_{w}d(T_{w^{\prime}}) for all w,wβ€²βˆˆWw,w^{\prime}\in W.

Since d2​(Ts)=0d^{2}(T_{s})=0 for s∈Ss\in S, it follows that by induction that d2=0d^{2}=0. ∎

The following corollary shows that the computation of d⁑(Tw)d(T_{w}) can be done using the Leibniz rule, given a reduced decomposition of ww. The terms that do not vanish are exactly the terms given in the original definition of d⁑(Tw)d(T_{w}).

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Corollary 3.1.4. Let w=si1β‹―silw=s_{i_{1}}\cdots s_{i_{l}} be a reduced expression of w∈Ww\in W. We have

d(Tw)=βˆ‘r=1lTi1β‹―Tirβˆ’1Tir+1Til.d(T_{w})=\sum_{r=1}^{l}T_{i_{1}}\cdots T_{i_{r-1}}T_{i_{r+1}}T_{i_{l}}.

We have Ti1β‹―Tirβˆ’1Tir+1Tilβ‰ 0T_{i_{1}}\cdots T_{i_{r-1}}T_{i_{r+1}}T_{i_{l}}\neq 0 if and only if si1β‹―sirβˆ’1sir+1β‹―sils_{i_{1}}\cdots s_{i_{r-1}}s_{i_{r+1}}\cdots s_{i_{l}} is reduced, i.e., if and only if β„“(si1β‹―sirβˆ’1sir+1β‹―sil)=β„“(w)βˆ’1\ell(s_{i_{1}}\cdots s_{i_{r-1}}s_{i_{r+1}}\cdots s_{i_{l}})=\ell(w)-1.

Given r,rβ€²r,r^{\prime} with si1β‹―sirβˆ’1sir+1β‹―sil=si1β‹―sirβ€²βˆ’1sirβ€²+1β‹―sils_{i_{1}}\cdots s_{i_{r-1}}s_{i_{r+1}}\cdots s_{i_{l}}=s_{i_{1}}\cdots s_{i_{r^{\prime}-1}}s_{i_{r^{\prime}+1}}\cdots s_{i_{l}} reduced, we have r=rβ€²r=r^{\prime}.

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Proof. The first statement follows from Proposition 3.1.3. The second statement is a property of the multiplication of TwT_{w}’s.

For the third statement, let us assume r<rβ€²r<r^{\prime}. We have sir+1β‹―sirβ€²=sirβ‹―sirβ€²βˆ’1s_{i_{r+1}}\cdots s_{i_{r^{\prime}}}=s_{i_{r}}\cdots s_{i_{r^{\prime}-1}} reduced, hence sirsir+1β‹―sirβ€²s_{i_{r}}s_{i_{r+1}}\cdots s_{i_{r^{\prime}}} is not reduced, a contradiction. ∎

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Remark 3.1.5. Note that the algebra Hnil​(W)H^{\mathrm{nil}}(W) is acyclic if Sβ‰ βˆ…S\neq\emptyset.

Note also that one can introduce a family of commuting differentials dsd_{s} for s∈Ss\in S modulo conjugacy by setting ds​(Tt)=1d_{s}(T_{t})=1 if t∈St\in S is conjugate to ss and ds​(Tt)=0d_{s}(T_{t})=0 otherwise.

The specialization over 𝐅2{\mathbf{F}}_{2} at as=bs=0a_{s}=b_{s}=0 of the bimodules L±​(I,J)L^{\pm}(I,J) of Β§3.1.3 acquire a structure of differential graded bimodules, using the differential graded structure of Hnil​(W)H^{\mathrm{nil}}(W). We keep the same notation for those differential graded specialized bimodules and for the maps tt and t^\hat{t}.

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Proposition 3.1.6. If WW is finite, then

tS,I:Hnil​(W)β†’Hnil​(WI)β€‹βŸ¨Nβˆ’NI⟩t_{S,I}:H^{\mathrm{nil}}(W)\to H^{\mathrm{nil}}(W_{I})\langle N-N_{I}\rangle

is a morphism of differential graded 𝐅2{\mathbf{F}}_{2}-modules and Corollary 3.1.2 provides an isomorphism of differential graded (Hnil​(WI),Hnil​(W))(H^{\mathrm{nil}}(W_{I}),H^{\mathrm{nil}}(W))-bimodules

t^S,IΒ±:Lβˆ“β€‹(I,S)β†’βˆΌL±​(S,I)βˆ¨β€‹βŸ¨Nβˆ’NI⟩.\hat{t}_{S,I}^{\pm}:L^{\mp}(I,S)\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}L^{\pm}(S,I)^{\vee}\langle N-N_{I}\rangle.
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Proof. Let v∈Wv\in W. There is a unique decomposition v=v′​vβ€²β€²v=v^{\prime}v^{\prime\prime} where ℓ⁑(v)=ℓ⁑(vβ€²)+ℓ⁑(vβ€²β€²)\ell(v)=\ell(v^{\prime})+\ell(v^{\prime\prime}), vβ€²β€²βˆˆWIv^{\prime\prime}\in W_{I} and vβ€²βˆˆWIv^{\prime}\in W^{I}.

We have d⁑(Tv)=d⁑(Tvβ€²)​Tvβ€²β€²+Tv′​d​(Tvβ€²β€²)d(T_{v})=d(T_{v^{\prime}})T_{v^{\prime\prime}}+T_{v^{\prime}}d(T_{v^{\prime\prime}}). If u∈Wu\in W and u<vβ€²u<v^{\prime}, then uβˆ‰wS​WIu{\not\in}w_{S}W_{I}. It follows that

tS,I​(d⁑(Tv))=tS,I​(Tv′​d​(Tvβ€²β€²))=Ξ΄vβ€²,wI​d​(Tvβ€²β€²)=d⁑(tS,I​(Tv)).t_{S,I}(d(T_{v}))=t_{S,I}(T_{v^{\prime}}d(T_{v^{\prime\prime}}))=\delta_{v^{\prime},w^{I}}d(T_{v^{\prime\prime}})=d(t_{S,I}(T_{v})).

∎

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2