ScalingStacks

3.1. Differential graded nil Hecke algebras

We discuss here the case of general Coxeter groups. The results will be used only for types AnA_{n} and A~n\tilde{A}_{n}.

3.1.1. Coxeter groups

We refer to [Hu, §5 and §7.1–7.3] for basic properties of Coxeter groups and Hecke algebras. Recall that a Coxeter group (W,S)(W,S) is the data of a group WW with a subset S⊂WS\subset W such that WW has a presentation with generating set SS and relations

s2=1,sts⋯⏟ms​t​ terms=tst⋯⏟ms​t​ terms​ when ​s​t​ has order ​ms​t​ for ​s,t∈S.s^{2}=1,\ \underbrace{sts\cdots}_{m_{st}\text{ terms}}=\underbrace{tst\cdots}_{m_{st}\text{ terms}}\text{ when }st\text{ has order }m_{st}\ \text{ for }s,t\in S.

A reduced expression of an element w∈Ww\in W is a decomposition w=si1⋯silw=s_{i_{1}}\cdots s_{i_{l}} such that sir∈Ss_{i_{r}}\in S for r=1,…,lr=1,\ldots,l and such that ll is minimal with this property. The integer ll is the length ℓ⁡(w)\ell(w) of ww.

The Chevalley-Bruhat (partial) order on WW is defined as follows. Let w′,w∈Ww^{\prime},w\in W and let w=si1⋯silw=s_{i_{1}}\cdots s_{i_{l}} be a reduced decomposition. We say that w′≤ww^{\prime}\leq w if there is l′≤ll^{\prime}\leq l and an increasing injection f:{1,…,l′}→{1,…,l}f:\{1,\ldots,l^{\prime}\}\to\{1,\ldots,l\} such that w′=sif⁡(1)⋯sif⁡(l′)w^{\prime}=s_{i_{f(1)}}\cdots s_{i_{f(l^{\prime})}}. This is independent of the choice of the reduced decomposition of ww.

3.1.2. Hecke algebras

Let R=𝐙⁡[{as,bs}s∈S]R={\mathbf{Z}}[\{a_{s},b_{s}\}_{s\in S}] where asa_{s} and bsb_{s} are indeterminates with as=as′a_{s}=a_{s^{\prime}} and bs=bs′b_{s}=b_{s^{\prime}} if ss and s′s^{\prime} are conjugate in WW.

The Hecke algebra H=H⁡(W)H=H(W) of (W,S)(W,S) is the RR-algebra generated by {Ts}s∈S\{T_{s}\}_{s\in S} with relations

Ts2+as​Ts+bs=0,TsTtTs⋯⏟ms​t​ terms=TtTsTt⋯⏟ms​t​ terms​ when ​s​t​ has order ​ms​t.T_{s}^{2}+a_{s}T_{s}+b_{s}=0,\ \underbrace{T_{s}T_{t}T_{s}\cdots}_{m_{st}\text{ terms}}=\underbrace{T_{t}T_{s}T_{t}\cdots}_{m_{st}\text{ terms}}\text{ when }st\text{ has order }m_{st}.

Given a reduced decomposition w=si1⋯silw=s_{i_{1}}\cdots s_{i_{l}}, we put Tw=Tsi1⋯TsilT_{w}=T_{s_{i_{1}}}\cdots T_{s_{i_{l}}}. This element is independent of the choice of the reduced decomposition of ww. The set {Tw}w∈W\{T_{w}\}_{w\in W} is a basis of HH.

Let ι:H→∼Hopp\iota:H\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}H^{\operatorname{opp}\nolimits} be the algebra automorphism defined by Ts↦TsT_{s}\mapsto T_{s} for s∈Ss\in S.

Let II be a subset of SS. We denote by WIW_{I} the subgroup of WW generated by II. The group WIW_{I}, together with II, is a Coxeter group and the length function on WIW_{I} is the restriction of that on WW [Hu, §1.10].

We put RI=𝐙⁡[{as,I,bs,I}s∈I]R_{I}={\mathbf{Z}}[\{a_{s,I},b_{s,I}\}_{s\in I}] where as,Ia_{s,I} and bs,Ib_{s,I} are indeterminates with as,I=as′,Ia_{s,I}=a_{s^{\prime},I} and bs,I=bs′,Ib_{s,I}=b_{s^{\prime},I} if ss and s′s^{\prime} are conjugate in WIW_{I}. There is a morphism of rings RI→R,as,I↦as,bs,I↦bsR_{I}\to R,\ a_{s,I}\mapsto a_{s},\ b_{s,I}\mapsto b_{s}.

We denote by HI=HI​(W)H_{I}=H_{I}(W) the RR-subalgebra of HH generated by {Ts}s∈I\{T_{s}\}_{s\in I}. There is an isomorphism of RR-algebras R⊗RIH⁡(WI)→∼HI​(W),Tw↦TwR\otimes_{R_{I}}H(W_{I})\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}H_{I}(W),\ T_{w}\mapsto T_{w}.

We assume for the remainder of §3.1.2 that WW is finite. In this case, there is a unique element wSw_{S} of WW with maximal length [Hu, §1.8] and we denote by NN its length. We have wS2=1w_{S}^{2}=1 and wS​S​wS=Sw_{S}Sw_{S}=S. There is an automorphism of algebras

ιS:H→∼H,Tv↦TwS⋅v⋅wS.\iota_{S}:H\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}H,\ T_{v}\mapsto T_{w_{S}\cdot v\cdot w_{S}}.

We denote by wIw_{I} the longest element of WIW_{I} and by NIN_{I} its length. We denote by WIW^{I} (resp. WI{{}^{I}W}) the set of elements v∈Wv\in W such that vv has minimal length in v​WIvW_{I} (resp. WI​vW_{I}v). Note that WI→∼W/WI,v↦v​WIW^{I}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}W/W_{I},\ v\mapsto vW_{I} [Hu, Proposition 1.10].

3.1.3. Traces

We assume in §3.1.3 that WW is finite.

Given J⊂IJ\subset I, we define an RR-linear map

tI,J:HI→HJ,Tv↦{TwJ​wI​v if ​v∈wI⋅WJ0 otherwise.t_{I,J}:H_{I}\to H_{J},\ T_{v}\mapsto\begin{cases}T_{w_{J}w_{I}v}&\text{ if }v\in w_{I}\cdot W_{J}\\ 0&\text{ otherwise.}\end{cases}

The next proposition shows this is relative Frobenius form (cf eg [Rou1, §2.3.2]).

0P4L

Proposition 3.1.1. We have tS,J=tI,J∘tS,It_{S,J}=t_{I,J}\circ t_{S,I}.

Given h∈Hh\in H and x∈WIx\in W_{I}, we have

tS,I​(h​Tx)=tS,I​(h)​Tx,tS,I​(TwS​wI⋅x⋅wI​wS​h)=Tx​tS,I​(h).t_{S,I}(hT_{x})=t_{S,I}(h)T_{x},\ t_{S,I}(T_{w_{S}w_{I}\cdot x\cdot w_{I}w_{S}}h)=T_{x}t_{S,I}(h).

Given h′∈Hh^{\prime}\in H commuting with HIH_{I}, we have tS,I​(h​h′)=tS,I​(ιS​(h′)​h)t_{S,I}(hh^{\prime})=t_{S,I}(\iota_{S}(h^{\prime})h).

There is an isomorphism of RR-modules

t^S,I:H→∼HomHIopp⁡(H,HI),h↦(h′↦tS,I​(h​h′))\hat{t}_{S,I}:H\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\operatorname{Hom}\nolimits_{H_{I}^{\operatorname{opp}\nolimits}}(H,H_{I}),\ h\mapsto(h^{\prime}\mapsto t_{S,I}(hh^{\prime}))

with

t^S,I​(TwS​wI⋅x⋅wI​wS​h​Ty)=Tx​t^S,I​(h)​Ty​ for ​x∈WI​ and ​y∈W.\hat{t}_{S,I}(T_{w_{S}w_{I}\cdot x\cdot w_{I}w_{S}}hT_{y})=T_{x}\hat{t}_{S,I}(h)T_{y}\text{ for }x\in W_{I}\text{ and }y\in W.
0P4M

Proof. Define wI=wS​wIw^{I}=w_{S}w_{I} and wI=wI​wS{{}^{I}w}=w_{I}w_{S}, so that wI⋅wI=1{{}^{I}w}\cdot w^{I}=1. We have wI∈WIw^{I}\in W^{I}.

Let v∈Wv\in W. There is a unique decomposition v=v′​v′′v=v^{\prime}v^{\prime\prime} where ℓ⁡(v)=ℓ⁡(v′)+ℓ⁡(v′′)\ell(v)=\ell(v^{\prime})+\ell(v^{\prime\prime}), v′′∈WIv^{\prime\prime}\in W_{I} and v′∈WIv^{\prime}\in W^{I} [Hu, Proposition 1.10]. Furthermore, ℓ⁡(v′)<ℓ⁡(wI)\ell(v^{\prime})<\ell(w^{I}) unless v′=wIv^{\prime}=w^{I}. We have tS,I​(Tv)=δv′,wI​Tv′′t_{S,I}(T_{v})=\delta_{v^{\prime},w^{I}}T_{v^{\prime\prime}}.

There is a unique decomposition v′′=v1​v2v^{\prime\prime}=v_{1}v_{2} with ℓ⁡(v′′)=ℓ⁡(v1)+ℓ⁡(v2)\ell(v^{\prime\prime})=\ell(v_{1})+\ell(v_{2}), v2∈WJv_{2}\in W_{J} and v1v_{1} has minimal length in v′′​WJv^{\prime\prime}W_{J}. We have v=(v′​v1)​v2v=(v^{\prime}v_{1})v_{2} where ℓ⁡(v)=ℓ⁡(v′​v1)+ℓ⁡(v2)\ell(v)=\ell(v^{\prime}v_{1})+\ell(v_{2}) and v′​v1v^{\prime}v_{1} has minimal length in v​WJvW_{J}. Furthermore, v′​v1=wJv^{\prime}v_{1}=w^{J} if and only if v′=wIv^{\prime}=w^{I} and v1=wI​wJv_{1}=w_{I}w_{J}. It follows that

tI,J∘tS,I​(Tv)=δv′,wI​tI,J​(Tv′′)=δv′,wI​δv1,wI​wJ​Tv2=tS,J​(Tv).t_{I,J}\circ t_{S,I}(T_{v})=\delta_{v^{\prime},w^{I}}t_{I,J}(T_{v^{\prime\prime}})=\delta_{v^{\prime},w^{I}}\delta_{v_{1},w_{I}w_{J}}T_{v_{2}}=t_{S,J}(T_{v}).

This shows the first statement of the lemma.

We have Tv′′​Tx∈HIT_{v^{\prime\prime}}T_{x}\in H_{I}, hence

tS,I​(Tv​Tx)=tS,I​(Tv′​(Tv′′​Tx))=δv′,wI​Tv′′​Tx=tS,I​(Tv)​Tx.t_{S,I}(T_{v}T_{x})=t_{S,I}(T_{v^{\prime}}(T_{v^{\prime\prime}}T_{x}))=\delta_{v^{\prime},w^{I}}T_{v^{\prime\prime}}T_{x}=t_{S,I}(T_{v})T_{x}.

This shows the second statement of the lemma.

Let x′=wI⋅x⋅wIx^{\prime}=w^{I}\cdot x\cdot{{}^{I}w}. We have ℓ⁡(wI⋅x⋅wI)=ℓ⁡(x)\ell(w^{I}\cdot x\cdot{{}^{I}w})=\ell(x). Since Tx′​TvT_{x^{\prime}}T_{v} is a linear combination of elements Ty​zT_{yz} with y≤x′y\leq x^{\prime} and z≤vz\leq v, it follows that if v′≠wIv^{\prime}\neq w^{I}, then Tx′​Tv′T_{x^{\prime}}T_{v^{\prime}} is a linear combination of elements TwI⋅y⋅wI​zT_{w^{I}\cdot y\cdot{{}^{I}w}z} with y∈WIy\in W_{I} and z∉wI​WIz{\not\in}w^{I}W_{I}, hence of elements TuT_{u} with u∉wI​WIu{\not\in}w^{I}W_{I}. So, if v′≠wIv^{\prime}\neq w^{I}, then tS,I​(Tx′​Tv)=0t_{S,I}(T_{x^{\prime}}T_{v})=0.

Assume now v′=wIv^{\prime}=w^{I}. We have Tx′​Tv=TwI⋅x⋅wI​TwI​Tv′′=TwI⋅x​Tv′′=TwI​Tx​Tv′′T_{x^{\prime}}T_{v}=T_{w^{I}\cdot x\cdot{{}^{I}w}}T_{w^{I}}T_{v^{\prime\prime}}=T_{w^{I}\cdot x}T_{v^{\prime\prime}}=T_{w^{I}}T_{x}T_{v^{\prime\prime}} because ℓ⁡(x′⋅wI)=ℓ⁡(wI⋅x)=ℓ⁡(wI)+ℓ⁡(x)=ℓ⁡(x′)+ℓ⁡(wI)\ell(x^{\prime}\cdot w^{I})=\ell(w^{I}\cdot x)=\ell(w^{I})+\ell(x)=\ell(x^{\prime})+\ell(w^{I}). We deduce that tS,I​(Tx′​Tv)=Tx​Tv′′=Tx​tS,I​(Tv)t_{S,I}(T_{x^{\prime}}T_{v})=T_{x}T_{v^{\prime\prime}}=T_{x}t_{S,I}(T_{v}). This shows the third statement of the lemma.

Let v0∈WIv_{0}\in W^{I}. We have ℓ⁡(wI)=ℓ⁡(wI​v0−1)+ℓ⁡(v0)\ell(w^{I})=\ell(w^{I}v_{0}^{-1})+\ell(v_{0}). Let v∈WIv\in W^{I}. Note that TwI​v0−1​Tv=TwI​v0−1​vT_{w^{I}v_{0}^{-1}}T_{v}=T_{w^{I}v_{0}^{-1}v} or TwI​v0−1​TvT_{w^{I}v_{0}^{-1}}T_{v} is a linear combination of TwT_{w}’s with ℓ⁡(w)<ℓ⁡(wI​v0−1)+ℓ⁡(v)\ell(w)<\ell(w^{I}v_{0}^{-1})+\ell(v). It follows that if tS,I​(TwI​v0−1​Tv)=0t_{S,I}(T_{w^{I}v_{0}^{-1}}T_{v})=0 if ℓ⁡(v)<ℓ⁡(v0)\ell(v)<\ell(v_{0}) or ℓ⁡(v)=ℓ⁡(v0)\ell(v)=\ell(v_{0}) and v≠v0v\neq v_{0}. We have also tS,I​(TwI​v0−1​Tv0)=1t_{S,I}(T_{w^{I}v_{0}^{-1}}T_{v_{0}})=1.

Since HH is a free right HIH_{I}-module with basis {Tv}v∈WI\{T_{v}\}_{v\in W^{I}}, we deduce that t^S,I\hat{t}_{S,I} is surjective. Since t^S,I\hat{t}_{S,I} is an RR-module morphism between free RR-modules of the same finite rank, it follows that it is an isomorphism. This shows the fifth statement of the lemma.

Let s∈Ss\in S and v∈Wv\in W. Let s′=wS⋅s⋅wS∈Ss^{\prime}=w_{S}\cdot s\cdot w_{S}\in S. If v∉{wS,wS⋅s}v{\not\in}\{w_{S},w_{S}\cdot s\}, then tS,∅​(Tv​Ts)=0t_{S,\emptyset}(T_{v}T_{s})=0 and tS,∅​(Ts′​Tv)=0t_{S,\emptyset}(T_{s^{\prime}}T_{v})=0. If v=wS⋅sv=w_{S}\cdot s, then Tv​Ts=TwS=Ts′​TvT_{v}T_{s}=T_{w_{S}}=T_{s^{\prime}}T_{v}. If v=wSv=w_{S}, then tS,∅​(Tv​Ts)=as=tS,∅​(Ts′​Tv)t_{S,\emptyset}(T_{v}T_{s})=a_{s}=t_{S,\emptyset}(T_{s^{\prime}}T_{v}). So, we have shown that tS,∅​(Tv​Ts)=tS,∅​(Ts′​Tv)t_{S,\emptyset}(T_{v}T_{s})=t_{S,\emptyset}(T_{s^{\prime}}T_{v}). It follows by induction on ℓ⁡(w)\ell(w) that tS,∅​(Tv​Tw)=tS,∅​(TwS⋅w⋅wS​Tv)t_{S,\emptyset}(T_{v}T_{w})=t_{S,\emptyset}(T_{w_{S}\cdot w\cdot w_{S}}T_{v}) for all w∈Ww\in W.

Consider now h′∈Hh^{\prime}\in H commuting with HIH_{I}. Let h′′∈HIh^{\prime\prime}\in H_{I}. We have

tI,∅​(tS,I​(h​h′)​h′′)=tI,∅​(tS,I​(h​h′​h′′))=tS,∅​(h​h′′​h′)=tS,∅​(ιS​(h′)​h​h′′)==tI,∅​(tS,I​(ιS​(h′)​h​h′′))=tI,∅​(tS,I​(ιS​(h′)​h)​h′′).t_{I,\emptyset}(t_{S,I}(hh^{\prime})h^{\prime\prime})=t_{I,\emptyset}(t_{S,I}(hh^{\prime}h^{\prime\prime}))=t_{S,\emptyset}(hh^{\prime\prime}h^{\prime})=t_{S,\emptyset}(\iota_{S}(h^{\prime})hh^{\prime\prime})=\\ =t_{I,\emptyset}(t_{S,I}(\iota_{S}(h^{\prime})hh^{\prime\prime}))=t_{I,\emptyset}(t_{S,I}(\iota_{S}(h^{\prime})h)h^{\prime\prime}).

It follows that t^I,∅​(tS,I​(h​h′))=t^I,∅​(tS,I​(ιS​(h′)​h))\hat{t}_{I,\emptyset}(t_{S,I}(hh^{\prime}))=\hat{t}_{I,\emptyset}(t_{S,I}(\iota_{S}(h^{\prime})h)), hence tS,I​(h​h′)=tS,I​(ιS​(h′)​h)t_{S,I}(hh^{\prime})=t_{S,I}(\iota_{S}(h^{\prime})h). This completes the proof of the lemma. ∎

We put tI,J+=tI,Jt^{+}_{I,J}=t_{I,J}. We define an RR-linear map

tI,J−:HI→HJ,Tv↦{Tv​wI​wJ if ​v∈WJ⋅wI0 otherwise.t^{-}_{I,J}:H_{I}\to H_{J},\ T_{v}\mapsto\begin{cases}T_{vw_{I}w_{J}}&\text{ if }v\in W_{J}\cdot w_{I}\\ 0&\text{ otherwise.}\end{cases}

We have tI,J−​(h)=ι⁡(tI,J+​(ι⁡(h)))t^{-}_{I,J}(h)=\iota(t^{+}_{I,J}(\iota(h))).

We put t^S,I+=t^S,I\hat{t}^{+}_{S,I}=\hat{t}_{S,I}. We have an isomorphism of RR-modules

t^S,I−:H→∼HomHIopp⁡(H,HI),h↦(h′↦tS,I−​(h​h′))\hat{t}^{-}_{S,I}:H\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}\operatorname{Hom}\nolimits_{H_{I}^{\operatorname{opp}\nolimits}}(H,H_{I}),\ h\mapsto(h^{\prime}\mapsto t^{-}_{S,I}(hh^{\prime}))

with

t^S,I−​(Tx​h​Ty)=Tx​t^S,I−​(h)​Ty​ for ​x∈WI​ and ​y∈W.\hat{t}_{S,I}^{-}(T_{x}hT_{y})=T_{x}\hat{t}_{S,I}^{-}(h)T_{y}\text{ for }x\in W_{I}\text{ and }y\in W.

Consider I,J⊂SI,J\subset S with I⊂JI\subset J or J⊂IJ\subset I. We define an (HI,HJ)(H_{I},H_{J})-bimodule L±​(I,J)L^{\pm}(I,J) with underlying RR-module HH. We put a=0a=0 if ±=+\pm=+ and a=1a=1 if ±=−\pm=-.

If I⊂JI\subset J, then the right action of HJH_{J} is by right multiplication and the left action of h∈HIh\in H_{I} is by left multiplication by (ιJ​ιI)a​(h)(\iota_{J}\iota_{I})^{a}(h).

If J⊂IJ\subset I, then the left action of HIH_{I} is by left multiplication and the right action of h∈HJh\in H_{J} is by right multiplication by (ιI​ιJ)a​(h)(\iota_{I}\iota_{J})^{a}(h).

Note that L±​(I,J)L^{\pm}(I,J) is free of finite rank as a left module and as a right module.

There is an isomorphism of (H,HI)(H,H_{I})-bimodules

L±​(I,S)∨=HomHopp⁡(L±​(I,S),H)→∼L±​(S,I),ζ↦ζ⁡(1).L^{\pm}(I,S)^{\vee}=\operatorname{Hom}\nolimits_{H^{\operatorname{opp}\nolimits}}(L^{\pm}(I,S),H)\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}L^{\pm}(S,I),\ \zeta\mapsto\zeta(1).

The next result follows immediately from Proposition 3.1.1.

0P4N

Corollary 3.1.2. The map t^S,I±\hat{t}^{\pm}_{S,I} is an isomorphism of (HI,H)(H_{I},H)-bimodules

L∓​(I,S)→∼L±​(S,I)∨=HomHIopp⁡(L±​(S,I),HI).L^{\mp}(I,S)\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}L^{\pm}(S,I)^{\vee}=\operatorname{Hom}\nolimits_{H_{I}^{\operatorname{opp}\nolimits}}(L^{\pm}(S,I),H_{I}).

The results above can be formulated in terms of dual bases. Note that {Tw}w∈WI\{T_{w}\}_{w\in W^{I}} is a basis of the free right HIH_{I}-module HH, while {Tw}w∈WI\{T_{w}\}_{w\in{{}^{I}W}} is a basis of the free left HIH_{I}-module HH.

We have

tS,I+​(TwS​wI​v−1​Tw)=δv,w​ and ​tS,I−​(Tv′​Tw′−1​wI​wS)=δv′,w′​ for ​v,w∈WI​ and ​v′,w′∈WI.t_{S,I}^{+}(T_{w_{S}w_{I}v^{-1}}T_{w})=\delta_{v,w}\text{ and }t_{S,I}^{-}(T_{v^{\prime}}T_{w^{\prime-1}w_{I}w_{S}})=\delta_{v^{\prime},w^{\prime}}\text{ for }v,w\in W^{I}\text{ and }v^{\prime},w^{\prime}\in{{}^{I}W}.

We deduce that the basis (TwS​wI​w−1)w∈WI(T_{w_{S}w_{I}w^{-1}})_{w\in W^{I}} when ±=+\pm=+ (resp. (Tw)w∈WI(T_{w})_{w\in{{}^{I}W}} when ±=−\pm=-) of the free left HIH_{I}-module L∓​(I,S)L^{\mp}(I,S) is dual to the basis (Tw)w∈WI(T_{w})_{w\in W^{I}} when ±=+\pm=+ (resp. (Tw−1​wI​wS)w∈WI(T_{w^{-1}w_{I}w_{S}})_{w\in{{}^{I}W}} when ±=−\pm=-) of the free right HIH_{I}-module L±​(S,I)L^{\pm}(S,I), via the pairing providing the isomorphism of Corollary 3.1.2.

The counit of the adjoint pair (L∓(I,S)⊗H−,L±(S,I)⊗HI−)(L^{\mp}(I,S)\otimes_{H}-,L^{\pm}(S,I)\otimes_{H_{I}}-) is given by the morphism of (HI,HI)(H_{I},H_{I})-bimodules

L∓​(I,S)⊗HL±​(S,I)→HI,a⊗b↦tS,I±​(a​b)L^{\mp}(I,S)\otimes_{H}L^{\pm}(S,I)\to H_{I},\ a\otimes b\mapsto t^{\pm}_{S,I}(ab)

while the unit is given by the morphism of (H,H)(H,H)-bimodules

H→L±​(S,I)⊗HIL∓​(I,S), 1↦{∑w∈WITw⊗TwS​wI​w−1 if ±=+∑w∈WITw−1​wI​wS⊗Tw if ±=−.H\to L^{\pm}(S,I)\otimes_{H_{I}}L^{\mp}(I,S),\ 1\mapsto\begin{cases}\sum_{w\in W^{I}}T_{w}\otimes T_{w_{S}w_{I}w^{-1}}&\text{ if }\pm=+\\ \sum_{w\in{{}^{I}W}}T_{w^{-1}w_{I}w_{S}}\otimes T_{w}&\text{ if }\pm=-.\end{cases}

3.1.4. Nil Hecke algebras

We define the nil Hecke algebra H𝐙nil​(W)H_{\mathbf{Z}}^{\mathrm{nil}}(W) of (W,S)(W,S) as the 𝐙{\mathbf{Z}}-algebra H⁡(W)⊗RR/(as,bs)s∈SH(W)\otimes_{R}R/(a_{s},b_{s})_{s\in S}. This is the 𝐙{\mathbf{Z}}-algebra generated by {Ts}s∈S\{T_{s}\}_{s\in S} with relations

Ts2=0,TsTtTs⋯⏟ms​t​ terms=TtTsTt⋯⏟ms​t​ terms​ when ​s​t​ has order ​ms​t.T_{s}^{2}=0,\ \underbrace{T_{s}T_{t}T_{s}\cdots}_{m_{st}\text{ terms}}=\underbrace{T_{t}T_{s}T_{t}\cdots}_{m_{st}\text{ terms}}\text{ when }st\text{ has order }m_{st}.

This is a 𝐙≤0{\mathbf{Z}}_{\leq 0}-graded algebra with TwT_{w} in degree −ℓ⁡(w)-\ell(w) for w∈Ww\in W.

The multiplication is given as follows:

(3.1.1) Tw​Tw′={Tw​w′ if ​ℓ​(w​w′)=ℓ⁡(w)+ℓ⁡(w′)0 otherwise.T_{w}T_{w^{\prime}}=\begin{cases}T_{ww^{\prime}}&\text{ if }\ell(ww^{\prime})=\ell(w)+\ell(w^{\prime})\\ 0&\text{ otherwise.}\end{cases}

Consider the filtration of the group algebra 𝐙⁡[W]{\mathbf{Z}}[W] where 𝐙​[W]≥−i{\mathbf{Z}}[W]^{\geq-i} is spanned by group elements w∈Ww\in W with ℓ⁡(w)≤i\ell(w)\leq i, for i∈𝐙≥0i\in{\mathbf{Z}}_{\geq 0}. The associated 𝐙≤0{\mathbf{Z}}_{\leq 0}-graded algebra is H𝐙nil​(W)H_{\mathbf{Z}}^{\mathrm{nil}}(W) and TwT_{w} is the image of w∈Ww\in W in the degree −ℓ⁡(w)-\ell(w) homogeneous component of H𝐙nil​(W)H_{\mathbf{Z}}^{\mathrm{nil}}(W).

3.1.5. Differential

Let Hnil​(W)=𝐅2⊗H𝐙nil​(W)H^{\mathrm{nil}}(W)={\mathbf{F}}_{2}\otimes H_{\mathbf{Z}}^{\mathrm{nil}}(W). We define a linear map d:Hnil​(W)→Hnil​(W)d:H^{\mathrm{nil}}(W)\to H^{\mathrm{nil}}(W) by

d⁡(Tw)=∑w′<w,ℓ⁡(w′)=ℓ⁡(w)−1Tw′.d(T_{w})=\sum_{w^{\prime}<w,\ \ell(w^{\prime})=\ell(w)-1}T_{w^{\prime}}.
0P4P

Proposition 3.1.3. The map dd defines a structure of differential graded algebra on Hnil​(W)H^{\mathrm{nil}}(W).

0P4Q

Proof. Let w∈Ww\in W and s∈Ss\in S with w​s>wws>w. We have d⁡(Tw​Ts)=d⁡(Tw​s)=∑w′<w​s,ℓ⁡(w′)=ℓ⁡(w)Tw′d(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]

{w′∈W|w′<ws,ℓ(w′)=ℓ(w)}={w′′s|w′′<w,w′′<w′′s,ℓ(w′′)=ℓ(w)−1}⊔{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​Tw′)=d⁡(Tw)​Tw′+Tw​d​(Tw′)d(T_{w}T_{w^{\prime}})=d(T_{w})T_{w^{\prime}}+T_{w}d(T_{w^{\prime}}) for all w,w′∈Ww,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}).

0P4R

Corollary 3.1.4. Let w=si1⋯silw=s_{i_{1}}\cdots s_{i_{l}} be a reduced expression of w∈Ww\in W. We have

d(Tw)=∑r=1lTi1⋯Tir−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 Ti1⋯Tir−1Tir+1Til≠0T_{i_{1}}\cdots T_{i_{r-1}}T_{i_{r+1}}T_{i_{l}}\neq 0 if and only if si1⋯sir−1sir+1⋯sils_{i_{1}}\cdots s_{i_{r-1}}s_{i_{r+1}}\cdots s_{i_{l}} is reduced, i.e., if and only if ℓ(si1⋯sir−1sir+1⋯sil)=ℓ(w)−1\ell(s_{i_{1}}\cdots s_{i_{r-1}}s_{i_{r+1}}\cdots s_{i_{l}})=\ell(w)-1.

Given r,r′r,r^{\prime} with si1⋯sir−1sir+1⋯sil=si1⋯sir′−1sir′+1⋯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=r′r=r^{\prime}.

0P4S

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<r′r<r^{\prime}. We have sir+1⋯sir′=sir⋯sir′−1s_{i_{r+1}}\cdots s_{i_{r^{\prime}}}=s_{i_{r}}\cdots s_{i_{r^{\prime}-1}} reduced, hence sirsir+1⋯sir′s_{i_{r}}s_{i_{r+1}}\cdots s_{i_{r^{\prime}}} is not reduced, a contradiction. ∎

0P4T

Remark 3.1.5. Note that the algebra Hnil​(W)H^{\mathrm{nil}}(W) is acyclic if S≠∅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 §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}.

0P4U

Proposition 3.1.6. If WW is finite, then

tS,I:Hnil​(W)→Hnil​(WI)​⟨N−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,I±:L∓​(I,S)→∼L±​(S,I)∨​⟨N−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.
0P4V

Proof. Let v∈Wv\in W. There is a unique decomposition v=v′​v′′v=v^{\prime}v^{\prime\prime} where ℓ⁡(v)=ℓ⁡(v′)+ℓ⁡(v′′)\ell(v)=\ell(v^{\prime})+\ell(v^{\prime\prime}), v′′∈WIv^{\prime\prime}\in W_{I} and v′∈WIv^{\prime}\in W^{I}.

We have d⁡(Tv)=d⁡(Tv′)​Tv′′+Tv′​d​(Tv′′)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<v′u<v^{\prime}, then u∉wS​WIu{\not\in}w_{S}W_{I}. It follows that

tS,I​(d⁡(Tv))=tS,I​(Tv′​d​(Tv′′))=δv′,wI​d​(Tv′′)=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})).

∎

3.1.6. Differential graded pointed Hecke monoid

Let WnilW^{\operatorname{nil}\nolimits} be the pointed 𝐙≤0{\mathbf{Z}}_{\leq 0}-graded monoid with underlying pointed set {Tw}w∈W​∐{0}\{T_{w}\}_{w\in W}\coprod\{0\} and multiplication given by (3.1.1). This is the pointed monoid gr⁡W{\operatorname{gr}\nolimits}W associated to the filtration on WW given by W≥−i={w∈W|ℓ⁡(w)≤i}W^{\geq-i}=\{w\in W\ |\ \ell(w)\leq i\} and there is an identification 𝐅2​[Wnil]=Hnil​(W){\mathbf{F}}_{2}[W^{\operatorname{nil}\nolimits}]=H^{\operatorname{nil}\nolimits}(W) making WnilW^{\operatorname{nil}\nolimits} into a differential graded pointed monoid.

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

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2