arXiv is now an independent nonprofit! Learn more
License: arXiv.org perpetual non-exclusive license
arXiv:1011.2010v2 [math.RT] 22 Mar 2011

Affine cellularity of affine Hecke algebras of rank two

Jérémie Guilhot and Vanessa Miemietz Address: Jérémie Guilhot: School of Mathematics, University of East Anglia Norwich NR4 7TJ, UK Email address: j.guilhot@uea.ac.uk Address: Vanessa Miemietz: School of Mathematics,
University of East Anglia Norwich NR4 7TJ, UK
Email address: v.miemietz@uea.ac.uk
Date: August 11, 2026
Abstract.

We show that affine Hecke algebras of rank two with generic parameters are affine cellular in the sense of Koenig-Xi.

1. Introduction

In order to approach the fundamental problem of classifying the irreducible representations of a given finite-dimensional algebra, the concept of cellularity, defined by Graham and Lehrer [5], has proven extremely useful. A cellular algebra comes, by definition, with a finite chain of ideals, whose subquotients, denoted by cells, decompose as left modules into a direct sum of copies of a certain module, called the cell module. This cell module comes with a bilinear form. Factoring out the radical with respect to this form leads to a simple module or zero, and in this way, one obtains a complete set of isomorphism classes of simple modules for the given cellular algebra. Examples of cellular algebras include many finite-dimensional Hecke algebras [4].

Recently, Koenig and Xi [9] have generalised this concept to algebras over a principal ideal domain kk of not necessarily finite dimension, by introducing the notion of an affine cellular algebra. Keeping the idea of having a filtration by a finite chain of ideals, the ideals are now allowed to be of infinite dimension. Where before a cell was isomorphic to a matrix ring over kk with a twisted multiplication, it is now isomorphic to a matrix ring (still of finite rank) over a quotient of a polynomial ring over kk, with a twisted multiplication. The most important class of examples in [9] of affine cellular algebras is given by the extended affine Hecke algebras of type AA.

In this article, we prove the following theorem, providing the first examples of affine cellularity for affine Hecke algebras with unequal parameters.

Theorem 1.1.

Let \mathcal{H} be an affine Hecke algebra of rank two defined over [v,v1]\mathbb{C}[v,v^{-1}] with generic parameters. Then \mathcal{H} is affine cellular in the sense of Koenig and Xi.

Theorem 1.1 is proved by explicit construction of the associated twisted matrix rings and the isomorphism between these and the corresponding cells.

2. Affine cellular algebras

Let kk be a principal ideal domain. For a kk-algebra AA, a kk-linear anti-automorphism ii of AA satisfying i2=idAi^{2}=id_{A} is called a kk-involution on AA. For two kk-modules V,WV,W denote by σ\sigma the map VkWWkVV\otimes_{k}W\rightarrow W\otimes_{k}V given by σ(vw)=wv\sigma(v\otimes w)=w\otimes v. If B=k[t1,,tr]/IB=k[t_{1},\dots,t_{r}]/I for some ideal II in a polynomial ring in finitely many variables over KK, then BB is called an affine kk-algebra.

Definition 2.1.

[9, Definition 2.1] Let AA be a unitary kk-algebra with a kk-involution ii. A two-sided ideal JJ in AA is called an affine cell ideal if and only if the following two conditions are satisfied.

  1. (1)

    We have i(J)=Ji(J)=J.

  2. (2)

    There exists an affine kk algebra BB with a kk-involution ν\nu, and a free kk-module VV of finite rank such that Δ:=VkB\Delta:=V\otimes_{k}B is an AA-BB-bimodule, where the right BB-structure is induced by the regular BB-module BBB_{B}.

  3. (3)

    There is an AA-AA-bimodule isomorphism α:JΔBΔ\alpha:J\rightarrow\Delta\otimes_{B}\Delta^{\prime}, where Δ=BkV\Delta^{\prime}=B\otimes_{k}V is the BB-AA-bimodule with left BB-structure induced by BB{}_{B}B and right AA structure defined by (bv)a=σ(i(a)(vb))(b\otimes v)a=\sigma(i(a)(v\otimes b)), such that the following diagram commutes:

    J\textstyle{J\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}α\scriptstyle{\alpha}i\scriptstyle{i}ΔBΔ\textstyle{\Delta\otimes_{B}\Delta^{\prime}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}vbBbwwν(b)Bν(b)v\scriptstyle{v\otimes b\otimes_{B}b^{\prime}\otimes w\mapsto w\otimes\nu(b^{\prime})\otimes_{B}\nu(b)\otimes v}J\textstyle{J\ignorespaces\ignorespaces\ignorespaces\ignorespaces}α\scriptstyle{\alpha}ΔBΔ.\textstyle{\Delta\otimes_{B}\Delta^{\prime}.}

The algebra AA together with its kk-involution ii is called affine cellular if and only if there is a kk-module decomposition A=J1J2JnA=J_{1}^{\prime}\oplus J_{2}^{\prime}\oplus\cdots\oplus J_{n}^{\prime} for some nn with i(Jl)=Jli(J_{l}^{\prime})=J_{l} for 1ln1\leq l\leq n, such that, setting Jm:=l=1mJlJ_{m}:=\bigoplus_{l=1}^{m}J_{l}^{\prime}, we obtain a filtration

0=J0J1J2Jn=A0=J_{0}\subset J_{1}\subset J_{2}\subset\cdots\subset J_{n}=A

of AA by two-sided ideals, where each Jm=Jm/Jm1J_{m}^{\prime}=J_{m}/J_{m-1} is an affine cell ideal of A/Jm1A/J_{m-1} (with respect to the involution induced by ii on the quotient).

For an affine kk-algebra BB with a kk-involution ν\nu, a free kk-module VV of finite rank and a kk-bilinear form φ:V×VB\varphi:V\times V\rightarrow B, denote by 𝔸(V,B,φ)\mathbb{A}(V,B,\varphi) the (possibly non-unital) algebra given as a kk-module by VkBkVV\otimes_{k}B\otimes_{k}V, on which we impose the multiplication (v1b1w1)(v2b2w2):=v1b1φ(w1,v2)b2w2(v_{1}\otimes b_{1}\otimes w_{1})(v_{2}\otimes b_{2}\otimes w_{2}):=v_{1}\otimes b_{1}\varphi(w_{1},v_{2})b_{2}\otimes w_{2}.

The description of affine cell ideal we are going to use is the following:

Proposition 2.2.

[9, Proposition 2.3] Let kk be a principal ideal domain, AA a unitary kk-algebra with a kk-involution ii. A two-sided ideal JJ in AA is an affine cell ideal if and only if there exists an affine kk-algebra BB with a kk-involution ν\nu, a free kk-module VV of finite rank and a bilinear form φ:VVB\varphi:V\otimes V\rightarrow B, and an AA-AA-bimodule structure on VkBkVV\otimes_{k}B\otimes_{k}V, such that J𝔸(V,B,φ)J\cong\mathbb{A}(V,B,\varphi) as an algebra and an AA-AA-bimodule, and such that under this isomorphism the kk-involution ii restricted to JJ corresponds to the kk-involution given by vbwwν(b)vv\otimes b\otimes w\mapsto w\otimes\nu(b)\otimes v.

Let now AA be an affine cellular algebra with a cell chain 0=J0J1J2Jn=A0=J_{0}\subset J_{1}\subset J_{2}\subset\cdots\subset J_{n}=A, such that each subquotient Ji/Ji1J_{i}/J_{i-1} is an affine cell ideal in A/Ji1A/J_{i-1}. Then Ji/Ji1J_{i}/J_{i-1} is isomorphic to 𝔸(Vi,Bi,φi)\mathbb{A}(V_{i},B_{i},\varphi_{i}) for some finite-dimensional vector space ViV_{i}, a commutative kk-algebra BiB_{i} and a bilinear form φi:Vi×ViBi\varphi_{i}:V_{i}\times V_{i}\rightarrow B_{i}. Let (ϕsti)(\phi^{i}_{st}) be the matrix representing the bilinear form ϕ\phi with respect to some choice of basis of ViV_{i}. Then Koenig and Xi obtain a parameterisation of simple modules over an affine cellular algebra by establishing a bijection between isomorphism classes of simple AA-modules and the set

{(j,m)1jn,mMaxSpec(Bj) such that some ϕstjm}\{(j,\mathrm{m})\mid 1\leq j\leq n,\mathrm{m}\in\mathrm{MaxSpec}(B_{j})\textrm{ such that some }\phi^{j}_{st}\not\in\mathrm{m}\}

where MaxSpec(Bj)\mathrm{MaxSpec}(B_{j}) denotes the maximal ideal spectrum of BjB_{j}. Furthermore, assume that Ji/Ji1J_{i}/J_{i-1} is an idempotent ideal in A/Ji1A/J_{i-1} (meaning (Ji/Ji1)2=Ji/Ji1(J_{i}/J_{i-1})^{2}=J_{i}/J_{i-1}), that it contains an idempotent in A/Ji1A/J_{i-1} and that the radical of every BjB_{j} is zero. Then, Koenig and Xi show that AA has finite global dimension if and only if every BiB_{i} has finite global dimension.

3. Hecke algebras and Kazhdan-Lusztig cells

In this section (W,S)(W,S) denotes an arbitrary Coxeter system (with |S|<|S|<\infty) together with a positive weight function LL. A positive weight function is a function L:WL:W\rightarrow\mathbb{N} such that L(ww)=L(w)+L(w)L(ww^{\prime})=L(w)+L(w^{\prime}) whenever (ww)=(w)+(w)\ell(ww^{\prime})=\ell(w)+\ell(w^{\prime}) where \ell denotes the usual length function on WW. The main reference is [11].

3.1. Hecke algebras and Kazhdan-Lusztig basis

Let 𝒜=[v,v1]\mathcal{A}=\mathbb{C}[v,v^{-1}] where vv is an indeterminate. Let \mathcal{H} be the Iwahori-Hecke algebra associated to WW, with 𝒜\mathcal{A}-basis {Tw|wW}\{T_{w}|w\in W\} and multiplication rule given by

TsTw={Tsw,if (sw)>(w),Tsw+(vL(s)vL(s))Tw,if (sw)<(w),T_{s}T_{w}=\begin{cases}T_{sw},&\mbox{if }\ell(sw)>\ell(w),\\ T_{sw}+(v^{L(s)}-v^{-L(s)})T_{w},&\mbox{if }\ell(sw)<\ell(w),\end{cases}

for all sSs\in S and wWw\in W. Let ¯\bar{\ } be the ring involution of 𝒜\mathcal{A} which takes vv to v1v^{-1}. It can be extended to a ring involution of \mathcal{H} via

wWawTw¯=wWa¯wTw11(aw𝒜).\overline{\sum_{w\in W}a_{w}T_{w}}=\sum_{w\in W}\bar{a}_{w}T_{w^{-1}}^{-1}\quad(a_{w}\in\mathcal{A}).

We set

𝒜<0=v1[v1] and <0=wW𝒜<0Tw.\begin{array}[]{ccccccc}\mathcal{A}_{<0}&=v^{-1}\mathbb{Z}[v^{-1}]&\text{ and }&\mathcal{H}_{<0}=\bigoplus_{w\in W}\mathcal{A}_{<0}T_{w}.\end{array}

For each wWw\in W there exists a unique element CwC_{w}\in\mathcal{H} (see [11, Theorem 5.2]) such that

  1. (1)

    C¯w=Cw\bar{C}_{w}=C_{w}

  2. (2)

    CwTwmod<0C_{w}\equiv T_{w}\mod\mathcal{H}_{<0}.

For any wWw\in W we set

Cw=Tw+yWPy,wTywhere Py,w𝒜<0.C_{w}=T_{w}+\sum_{y\in W}P_{y,w}T_{y}\quad\text{where $P_{y,w}\in\mathcal{A}_{<0}$}.

It is well known ([11, §5.3]) that Py,w=0P_{y,w}=0 whenever ywy\nleq w (here \leq denotes the Bruhat order). It follows that {Cw|wW}\{C_{w}|w\in W\} forms an 𝒜\mathcal{A}-basis of \mathcal{H} (the “Kazhdan-Lusztig basis”). The coefficients Py,wP_{y,w} are known as the Kazhdan-Lusztig polynomials.

Definition 3.1.

Following Lusztig [11, §3.4], there exists a unique involutive antiautomorphism, i.e. an 𝒜\mathcal{A}-involution, :\flat:\mathcal{H}\longrightarrow\mathcal{H} which carries TwT_{w} to Tw1T_{w^{-1}}.

Remark 3.2.

Using this map, we obtain right handed version of the multiplication of \mathcal{H}:

TwTs={Tws,if (ws)>(w),Tws+(vL(s)vL(s))Tw,if (ws)<(w).T_{w}T_{s}=\begin{cases}T_{ws},&\mbox{if }\ell(ws)>\ell(w),\\ T_{ws}+(v^{L(s)}-v^{-L(s)})T_{w},&\mbox{if }\ell(ws)<\ell(w).\end{cases}

Further, since \flat sends <0\mathcal{H}_{<0} to itself it can be shown that [11, §5.6] that Cw=Cw1C_{w}^{\flat}=C_{w^{-1}}, from where it follows that

Py,w=Py1,w1.P_{y,w}=P_{y^{-1},w^{-1}}.

3.2. Kazhdan-Lusztig cells

We denote by hx,y,zh_{x,y,z} the structure constant with respect to the Kazhdan-Lusztig basis. That is, we set

CxCy=zWhx,y,zCz.C_{x}C_{y}=\sum_{z\in W}h_{x,y,z}C_{z}.

Note that h¯x,y,z=hx,y,z\bar{h}_{x,y,z}=h_{x,y,z} and, similarly to Remark 3.2, we have hx,y,z=hy1,x1,z1h_{x,y,z}=h_{y^{-1},x^{-1},z^{-1}}. We write zyz\leftarrow_{\mathcal{L}}y if there exists some sSs\in S such that hs,y,z0h_{s,y,z}\neq 0, that is CzC_{z} appears with a non-zero coefficient in the expression of CsCyC_{s}C_{y} in the Kazhdan-Lusztig basis. The Kazhdan-Lusztig left pre-order \leq_{\mathcal{L}} on WW is the transitive closure of this relation. The equivalence relation associated to \leq_{\mathcal{L}} will be denoted by \sim_{\mathcal{L}}, that is

xyxy and yx(x,yW).x\sim_{\mathcal{L}}y\Longleftrightarrow x\leq_{\mathcal{L}}y\text{ and }y\leq_{\mathcal{L}}x\quad(x,y\in W).

The corresponding equivalence classes are called the left cells of WW. Similarly, we can define a pre-order \leq_{\mathcal{R}} multiplying on the right in the defining relation. The associated equivalence relation will be denoted by \sim_{\mathcal{R}} and the corresponding equivalence classes are called the right cells of WW. Using the antiautomorphism \flat, we have (see [11, §8])

xyx1y1.x\leq_{\mathcal{L}}y\Longleftrightarrow x^{-1}\leq_{\mathcal{R}}y^{-1}.

Finally we write xyx\leq_{\mathcal{LR}}y if there exists a sequence x=x0,x1,,xn=yx=x_{0},x_{1},...,x_{n}=y of WW such that for each 0in10\leq i\leq n-1 we have either xixi+1x_{i}\leftarrow_{\mathcal{L}}x_{i+1} or xixi+1x_{i}\leftarrow_{\mathcal{R}}x_{i+1}. The equivalence relation associated to \leq_{\mathcal{LR}} will be denoted by \sim_{\mathcal{LR}} and the equivalence classes are called the two-sided cells of WW.
The preorders ,,\leq_{\mathcal{L}},\leq_{\mathcal{R}},\leq_{\mathcal{LR}} induce partial orders on the left, right and two-sided cells, respectively.

3.3. Kazhdan-Lusztig cell modules

We will follow the notation of [1]. Let ?{,,}?\in\{\mathcal{L},\mathcal{R},\mathcal{LR}\}. We define a ??-ideal to be a left ideal if ?=?=\mathcal{L}, a right ideal if ?=R?=R and a two-sided ideal if ?=?=\mathcal{LR}. Similarly, an \mathcal{H}-?-module is a left \mathcal{H}-module if ?=?=\mathcal{L}, a right \mathcal{H}-module if ?=R?=R and an \mathcal{H}-\mathcal{H}-bimodule if ?=?=\mathcal{LR}.

Let Γ\Gamma be a ??-cell of WW. We set

?Γ=𝒽Cyy?w,wΓ𝒾𝒜 and <?Γ=𝒽Cyy<?w,wΓ𝒾𝒜.\begin{array}[]{rllcc}\mathcal{H}_{\leq_{?}\Gamma}&=\mathcal{h}C_{y}\mid y\leq_{?}w,w\in\Gamma\mathcal{i}_{\mathcal{A}}\text{ and }\\ \mathcal{H}_{<_{?}\Gamma}&=\mathcal{h}C_{y}\mid y<_{?}w,w\in\Gamma\mathcal{i}_{\mathcal{A}}.\\ \end{array}

Then by definition of ?\leq_{?}, we see that ?Γ\mathcal{H}_{\leq_{?}\Gamma} and <?Γ\mathcal{H}_{<_{?}\Gamma} are ??-ideals of \mathcal{H}. Therefore

?Γ:=?Γ/<?Γ\mathcal{M}^{?}_{\Gamma}:=\mathcal{H}_{\leq_{?}\Gamma}/\mathcal{H}_{<{?}\Gamma}

is naturally an \mathcal{H}-??-module. It is called the Kazhdan-Lusztig cell module associated to Γ\Gamma. Note that it is a free 𝒜\mathcal{A}-module with basis the images of the elements CwC_{w} for wΓw\in\Gamma.

Let Γ\Gamma be a two-sided cell of WW and let

Γ=i=1mΓi\Gamma=\bigcup^{m}_{i=1}\Gamma_{i}

be its decomposition into left cells. We denote by [.][\ .\ ] the natural projection onto Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma}. (Then Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} has an 𝒜\mathcal{A}-basis {[Cw]wΓ}\{[C_{w}]\mid w\in\Gamma\}.) As an 𝒜\mathcal{A}-module we have

Γi=1mΓi.\mathcal{M}^{\mathcal{LR}}_{\Gamma}\cong\bigoplus_{i=1}^{m}\mathcal{M}^{\mathcal{L}}_{\Gamma_{i}}.

Further if one assumes that the Lusztig conjecture

(\ast) xy and xyxyx\leq_{\mathcal{L}}y\text{ and }x\sim_{\mathcal{LR}}y\Longrightarrow x\sim_{\mathcal{L}}y

holds, then the 𝒜\mathcal{A}-submodules Γi\mathcal{M}^{\mathcal{L}}_{\Gamma_{i}} are left \mathcal{H}-submodules of Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} for all 1im1\leq i\leq m. Indeed, for all hh\in\mathcal{H} and yΓiy\in\Gamma_{i}, we have

hCy=zyazCz=zy,zΓazCz+zy,zΓazCzfor some az𝒜hC_{y}=\sum_{z\leq_{\mathcal{L}}y}a_{z}C_{z}=\sum_{z\leq_{\mathcal{L}}y,z\in\Gamma}a_{z}C_{z}+\sum_{z\leq_{\mathcal{L}}y,z\notin\Gamma}a_{z}C_{z}\quad\text{for some $a_{z}\in\mathcal{A}$}

which, using ()(\ast), yields that h[Cy]Γih[C_{y}]\in\mathcal{M}^{\mathcal{L}}_{\Gamma_{i}}.

Remark 3.3.

Conjecture ()(\ast) is known to hold in the equal parameter case. In [8] it is shown that it holds in affine Weyl groups of rank 2 for all choices of parameters.

Finally, since the \mathcal{H}-\mathcal{H}-bimodule Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} is a two-sided ideal in /<Γ\mathcal{H}/\mathcal{H}_{<_{\mathcal{LR}}\Gamma}, it can be viewed as an algebra (possibly without identity element). The multiplication is given by

[Cx][Cy]=[CxCy]=zΓhx,y,z[Cz].[C_{x}][C_{y}]=[C_{x}C_{y}]=\sum_{z\in\Gamma}h_{x,y,z}[C_{z}].

If one assumes that ()(\ast) holds, then the 𝒜\mathcal{A}-submodules Γi\mathcal{M}^{\mathcal{L}}_{\Gamma_{i}} are left ideals of Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} for all 1im1\leq i\leq m.

Remark 3.4.

Note that the involution \flat fixes each Γ\mathcal{H}_{\leq_{\mathcal{LR}}\Gamma} and <Γ\mathcal{H}_{<_{\mathcal{LR}}\Gamma} hence induces an involution on Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma}. We will still denote this involution by \flat.

3.4. Generic parameters

Let S¯={𝐬¯1,,𝐬¯r}\bar{S}=\{\bar{{\bf s}}_{1},...,\bar{{\bf s}}_{r}\} be the set of conjugacy classes in SS. Any weight function on WW is completely determined by its values on S¯\bar{S}. Let V=rV=\mathbb{R}^{r} be the Euclidean space of dimension rr and let ω1,,ωr\omega_{1},...,\omega_{r} be the standard basis of VV. We identify the set of weight functions on WW with the set of points in VV with integer coordinates via

L(L(s1),,L(sr))VL\longrightarrow(L(s_{1}),...,L(s_{r}))\in V

where si𝐬¯is_{i}\in\bar{{\bf s}}_{i} for all ii. The element of the rr-tuple (L(s1),,L(sr))(L(s_{1}),...,L(s_{r})) are called the parameters. To any choice of parameters one can associate a partition of WW into left, right and two-sided cells.

According to Bonnafé’s semicontinuity conjecture [1], there exists a minimal finite set of hyperplanes \mathfrak{H} in VV such that the partition of WW into cells is the same for all parameters 𝒫,𝒫r\mathcal{P},\mathcal{P}^{\prime}\in\mathbb{N}^{r} belonging to the same \mathfrak{H}-facet (we refer to [2] for the definition of facets). The elements of this minimal set are called essential hyperplanes. The conjecture also states that the partition into cells for non-generic parameters can be recovered from the partition with respect to generic parameters. We refer to [1] for details on this conjecture. In the following definition we assume that Bonnafé’s conjecture holds.

Definition 3.5.

The parameters 𝒫:=(a1,,ar)r\mathcal{P}:=(a_{1},\ldots,a_{r})\in\mathbb{N}^{r} are called generic if they do not belong to any essential hyperplane for WW.

In this paper, we are only concerned with affine Weyl groups of rank 2 where the semicontinuity conjecture is known to hold and where the generic parameters have been determined in [8].

Example 3.6.

Let (W,S)(W,S) be the affine Weyl group of type G~2\tilde{G}_{2} with diagram and weight function given by

where a,ba,b are positive integers. Then (a,b)2(a,b)\in\mathbb{N}^{2} is generic if and only if a/b1, 3/2, 2a/b\neq 1,\ 3/2,\ 2. The corresponding partition into cells can be found in [8].

Example 3.7.

Let (W,S)(W,S) be the affine Weyl group of type B~2\tilde{B}_{2} with diagram and weight function given by

where a,b,ca,b,c are positive integers. We define the following hyperplanes in 2\mathbb{R}^{2}

0,-0.3)(5.5,5.3) 0,0)(5,5)

Then (a,b,c)3(a,b,c)\in\mathbb{N}^{3} is generic if and only if (a/b,c/b)(a/b,c/b) does not belong to any hyperplanes on the picture above [8, 6]. The corresponding partition into cells can be found in [6].

3.5. On the induction of Kazhdan-Lusztig cells

In this section we introduce the relative Kazhdan-Lusztig polynomials as in [3]. Let SSS^{\prime}\subsetneq S. We denote by WW^{\prime} the subgroup of WW generated by SS^{\prime} and by XX^{\prime} the set of distinguished left coset representative of WW^{\prime} in WW. Every element of wWw\in W can be written uniquely w=xuw=xu where xXx\in X^{\prime} and uWu\in W^{\prime}. Note that (w)=(x)+(u)\ell(w)=\ell(x)+\ell(u).
Let \preceq^{\prime} be the Kazhdan-Lusztig left preorder relation defined with respect to the Coxeter group (W,S)(W^{\prime},S^{\prime}) and the corresponding Hecke algebra. We define a relation \sqsubseteq on WW as follows. Let x,yXx,y\in X^{\prime} and u,vWu,v\in W^{\prime}. We write xuyvxu\sqsubset yv if x<yx<y and uvu\preceq v. We write xuyvxu\sqsubseteq yv if xuyvxu\sqsubset yv or x=yx=y and u=vu=v. Then we have

Proposition 3.8.

([3, Proposition 3.3]) For any yXy\in X^{\prime} and vWv\in W^{\prime} we have

Cyv=xX,uWxuyvpxu,yvTxCuC_{yv}=\underset{xu\sqsubseteq yv}{\sum_{x\in X^{\prime},u\in W^{\prime}}}p^{*}_{xu,yv}T_{x}C_{u}

where pyv,yv=1p^{*}_{yv,yv}=1 and pxu,yv𝐀<0p_{xu,yv}\in\mathbf{A}_{<0} if xuyvxu\sqsubset yv.

Remark 3.9.

Recall the 𝒜\mathcal{A}-involution :\flat:\mathcal{H}\rightarrow\mathcal{H} from Definition 3.1, which can be used to obtain a right-handed version of the above result. First Y=X1Y^{\prime}=X^{\prime-1} is the set of distinguished right coset representative of WW^{\prime} in WW. Any wWw\in W can be uniquely written w=uxw=ux where uWu\in W^{\prime} and xYx\in Y^{\prime}. We get for all yYy\in Y^{\prime} and vWv\in W^{\prime}:

Cvy=xY,uWuxvypux,vy,rCuTxC_{vy}=\underset{ux\sqsubseteq_{\mathcal{R}}vy}{\sum_{x\in Y^{\prime},u\in W^{\prime}}}p^{\ast,r}_{ux,vy}C_{u}T_{x}

where pux,vy,r=p(ux)1,(yv)1p^{\ast,r}_{ux,vy}=p^{\ast}_{(ux)^{-1},(yv)^{-1}}.

Using this theorem, Geck obtained the following result (see [3, Section 4]).

Corollary 3.10.

Let 𝔟\mathfrak{b} be a left ideal of WW^{\prime} with respect to \leq^{\prime}_{\mathcal{L}}. Then the set X𝔟X^{\prime}\mathfrak{b} is a left ideal of WW with respect to \leq_{\mathcal{L}}.

3.6. Generalised induction of Kazhdan-Lusztig cells

We now introduce the Generalised Induction Theorem. The idea is to generalise the construction above to some subsets of WW which may not be parabolic subgroups. We refer to [7, 8] for details.

We consider a subset UWU\subseteq W and a collection {Xu|uU}\{X_{u}\ |\ u\in U\} of subsets of WW satisfying the following conditions

  1. I1.

    for all uUu\in U, we have eXue\in X_{u},

  2. I2.

    for all uUu\in U and xXux\in X_{u} we have (xu)=(x)+(u)\ell(xu)=\ell(x)+\ell(u),

  3. I3.

    for all u,vUu,v\in U such that uvu\neq v we have XuuXvv=X_{u}u\cap X_{v}v=\emptyset,

  4. I4.

    the submodule :=𝒽TxCu|uU,xXu𝒾𝒜\mathcal{M}:=\mathcal{h}T_{x}C_{u}|\ u\in U,\ x\in X_{u}\mathcal{i}_{\mathcal{A}}\subseteq\mathcal{H} is a left ideal.

One can easily see that the set :={TxCu|uU,xXu}\mathcal{B}:=\{T_{x}C_{u}|u\in U,x\in X_{u}\} is an 𝒜\mathcal{A}-basis of \mathcal{M}. Thus for all yWy\in W and all vUv\in U, we can write

TyCv=uU,xXuax,uTxCufor some ax,u𝒜.T_{y}C_{v}=\sum_{u\in U,x\in X_{u}}a_{x,u}T_{x}C_{u}\quad\text{for some $a_{x,u}\in\mathcal{A}$}.

Let \preceq be the relation on UU defined as follows. Let u,vUu,v\in U. We write uvu\preceq v if there exist yWy\in W and xXux\in X_{u} such that TxCuT_{x}C_{u} appears with a non-zero coefficient in the expression of TyCvT_{y}C_{v} in the basis \mathcal{B}. We still denote by \preceq the pre-order induced by this relation (i.e. the transitive closure). For u,vUu,v\in U, xXux\in X_{u} and yXvy\in X_{v} we write xuyvxu\sqsubset yv if uvu\preceq v and xu<yvxu<yv. We write xuyvxu\sqsubseteq yv if xuyvxu\sqsubset yv or x=yx=y and u=vu=v.

Proposition 3.11.

([7, Proposition 3.8]) For any vUv\in U and yXuy\in X_{u}, there exist a unique family of polynomials (pxu,yv)xuyv(p^{*}_{xu,yv})_{xu\sqsubset yv} in 𝐀<0\mathbf{A}_{<0} such that

C~yv:=TyCv+uU,xXuxuyvpxu,yvTxCu\tilde{C}_{yv}:=T_{y}C_{v}+\underset{xu\sqsubset yv}{\sum_{u\in U,x\in X_{u}}}p^{*}_{xu,yv}T_{x}C_{u}

is stable under the ¯\bar{\ } involution.

Now if one assumes that

  1. I5.

    for all vUv\in U, yXvy\in X_{v} we have

    TyCvTyvmod<0T_{y}C_{v}\equiv T_{yv}\mod\mathcal{H}_{<0}

then we have C~yv=Cyv\tilde{C}_{yv}=C_{yv}.

Remark 3.12.

This is really a generalisation of Geck’ s result. If we set U=WU=W^{\prime} and Xu=XX_{u}=X^{\prime} for all uUu\in U then condition I1I4 are satisfied. For condition I5 we have for vWv\in W^{\prime} and yXy\in X^{\prime}:

C~yv\displaystyle\tilde{C}_{yv} =TyCv+uU,xXuxuyvpxu,yvTxCu\displaystyle=T_{y}C_{v}+\underset{xu\sqsubset yv}{\sum_{u\in U,x\in X_{u}}}p^{*}_{xu,yv}T_{x}C_{u}
=Ty(Tv+v1<vPv1,vTv1)+uU,xXuxuyvpxu,yvTxu1uPu1,uTu1\displaystyle=T_{y}\big(T_{v}+\sum_{v_{1}<v}P_{v_{1},v}T_{v_{1}}\big)+\underset{xu\sqsubset yv}{\sum_{u\in U,x\in X_{u}}}p^{*}_{xu,yv}T_{x}\sum_{u_{1}\leq u}P_{u_{1},u}T_{u_{1}}
=Tyv+(v1<vPv1,vTyTv1)+uU,xXuxuyvu1upxu,yvPu1,uTxTu1\displaystyle=T_{yv}+\big(\sum_{v_{1}<v}P_{v_{1},v}T_{y}T_{v_{1}}\big)+\underset{xu\sqsubset yv}{\sum_{u\in U,x\in X_{u}}}\sum_{u_{1}\leq u}p^{*}_{xu,yv}P_{u_{1},u}T_{x}T_{u_{1}}
=Tyv+(v1<vPv1,vTyv1)+uU,xXuxuyvu1upxu,yvPu1,uTxu1\displaystyle=T_{yv}+\big(\sum_{v_{1}<v}P_{v_{1},v}T_{yv_{1}}\big)+\underset{xu\sqsubset yv}{\sum_{u\in U,x\in X_{u}}}\sum_{u_{1}\leq u}p^{*}_{xu,yv}P_{u_{1},u}T_{xu_{1}}
Tyvmod<0.\displaystyle\equiv T_{yv}\mod\mathcal{H}_{<0}.

Since C~yv\tilde{C}_{yv} is stable under the involution ¯\bar{\ } we get C~yv=Cyv\tilde{C}_{yv}=C_{yv}.

4. Main result

Throughout this section, WW denotes an affine Weyl group of rank 2 and LL a generic weight function. We fix a two-sided cell Γ\Gamma of WW and wish to show that Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} is an affine cell ideal in /<Γ\mathcal{H}/\mathcal{H}_{<_{\mathcal{LR}}\Gamma}. In Sections 4.14.4, we assume that, in the case where WW is of type G~2\tilde{G}_{2}, the two-sided cell Γ\Gamma is either infinite or does not intersect the group generated by s2,s3s_{2},s_{3}. The remaining cases will be treated in Section 4.5.

4.1. Description of Γ\Gamma

In this section we present a very nice description of Γ\Gamma. It is rather surprising that most of the two-sided cells in WW can be described in such a uniform way. Note that this description is vital in the proof of affine cellularity. We refer to the next section for examples of this description.

By inspection of the different partitions into cells given in [6, 8], one can show that there exist two subsets 𝒯\mathcal{T} and 𝒵={z1=e,z2,,zm}\mathcal{Z}=\{z_{1}=e,z_{2},\ldots,z_{m}\} of WW and an element wΓWw_{\Gamma}\in W in a parabolic subgroup WW^{\prime} such that for all 1i,jm1\leq i,j\leq m and all τ𝒯\tau\in\mathcal{T} we have

(zi1τwΓzk)=(zi1)+(τ)+(wΓ)+(zj)\ell(z_{i}^{-1}\tau w_{\Gamma}z_{k})=\ell(z_{i}^{-1})+\ell(\tau)+\ell(w_{\Gamma})+\ell(z_{j})

and the following map is bijective

𝒵×𝒯×𝒵Γ(zi,τ,zj)zi1τwΓzjΓi1Γj.\begin{array}[]{ccccccc}&\mathcal{Z}\times\mathcal{T}\times\mathcal{Z}&\longrightarrow&\Gamma&\\ &(z_{i},\tau,z_{j})&\longmapsto&z_{i}^{-1}\tau w_{\Gamma}z_{j}&\in\Gamma_{i}^{-1}\cap\Gamma_{j}.\end{array}

The left cells lying in Γ\Gamma are of the form

Γj={zi1τwΓzjτ𝒯,1im}.\Gamma_{j}=\{z_{i}^{-1}\tau w_{\Gamma}z_{j}\mid\tau\in\mathcal{T},1\leq i\leq m\}.

and we have

(Γi)1Γj={zi1τwΓzjτ𝒯}.(\Gamma_{i})^{-1}\cap\Gamma_{j}=\{z_{i}^{-1}\tau w_{\Gamma}z_{j}\mid\tau\in\mathcal{T}\}.

The set 𝒯\mathcal{T} can be expressed in one of the following forms:

  1. (1)

    𝒯={t1nt2mn,m}\mathcal{T}=\{t_{1}^{n}t_{2}^{m}\mid n,m\in\mathbb{N}\}

  2. (2)

    𝒯={tnn}\mathcal{T}=\{t^{n}\mid n\in\mathbb{N}\}

  3. (3)

    𝒯={e,t}\mathcal{T}=\{e,t\}

  4. (4)

    𝒯={e}\mathcal{T}=\{e\}

In case (1) we set T={t1,t2}T=\{t_{1},t_{2}\}, in case (2) and (3) we set T={t}T=\{t\} and in case (4) we set T={e}T=\{e\}. In all cases it can be checked that for τ𝒯\tau\in\mathcal{T}, we have

τwΓ=wΓτ1.\tau w_{\Gamma}=w_{\Gamma}\tau^{-1}.

It is clear that if Γ\Gamma is infinite, then we must be in case (1) or (2) and if Γ\Gamma is finite then we must be in case (3) or (4). We refer to Section 5 for examples of the different cases: when Γ=c~0\Gamma=\tilde{c}_{0} we are in case (1), when Γ=c~1\Gamma=\tilde{c}_{1} or c~2\tilde{c}_{2} we are in case (2), when Γ=c~3\Gamma=\tilde{c}_{3} we are in case (3) and when Γ=c~4\Gamma=\tilde{c}_{4} we are in case (4).

Remark 4.1.

This description is no longer true for all cells if the parameters are non-generic which is why in this paper we are only considering generic parameters.

4.2. The element 𝐏\mathbf{P}

Let XX^{\prime} be the set of distinguished left coset representative of WW^{\prime} in WW and let \leq^{{}^{\prime}}_{\mathcal{L}} be the Kazhdan-Lusztig left preorder relation defined with respect to WW^{\prime}. Then explicit computations show that either

  1. (1)

    wΓw_{\Gamma} is the longest element in WW^{\prime};

  2. (2)

    wΓ=sww_{\Gamma}=sw^{\prime} where ww^{\prime} is the longest element of WW^{\prime}, wΓ2=1w_{\Gamma}^{2}=1 and {wΓ,w}\{w_{\Gamma},w^{\prime}\} is a left ideal of WW^{\prime} with respect to \leq^{\prime}_{\mathcal{L}}.

The element 𝐏\mathbf{P} in Case (1). Assume we are in Case (1). By well-known properties of the longest element in a Coxeter group, for all uWu\in W^{\prime} we have uwΓu\leq^{\prime}_{\mathcal{L}}w_{\Gamma} implies that u=wΓu=w_{\Gamma}. Further, one can easily check from the definition of \sqsubset that this implies that if wWw\in W satisfies wywΓw\sqsubseteq yw_{\Gamma} then w=xwΓw=xw_{\Gamma} with x<yx<y and xXx\in X^{\prime}. Thus by Proposition 3.8 we get for all yXy\in X^{\prime}

CywΓ\displaystyle C_{yw_{\Gamma}} =TyCwΓ+x<y,xXpxwΓ,ywΓTzCwΓ\displaystyle=T_{y}C_{w_{\Gamma}}+\sum_{x<y,x\in X^{\prime}}p^{*}_{xw_{\Gamma},yw_{\Gamma}}T_{z}C_{w_{\Gamma}}
=(Ty+x<y,xXpxwΓ,ywΓTz)CwΓ.\displaystyle=\big(T_{y}+\sum_{x<y,x\in X^{\prime}}p^{*}_{xw_{\Gamma},yw_{\Gamma}}T_{z}\big)C_{w_{\Gamma}}.

We set for y𝒵1Ty\in\mathcal{Z}^{-1}\cup T

𝐏(y)=xy,xXpxwΓ,ywΓTx,𝐏𝐑(y1)=(𝐏(y)),\mathbf{P}(y)=\sum_{x\leq y,x\in X^{\prime}}p^{\ast}_{xw_{\Gamma},yw_{\Gamma}}T_{x},\quad\mathbf{P}_{\mathbf{R}}(y^{-1})=(\mathbf{P}(y))^{\flat},

so that we have

𝐏(y)CwΓ=CywΓ and CwΓ𝐏𝐑(y1)=CwΓy1.\mathbf{P}(y)C_{w_{\Gamma}}=C_{yw_{\Gamma}}\text{ and }C_{w_{\Gamma}}\mathbf{P}_{\mathbf{R}}(y^{-1})=C_{w_{\Gamma}y^{-1}}.

The last equality holds since

CwΓ𝐏𝐑(y1)=CwΓ(𝐏(y))=(𝐏(y)CwΓ)=(CywΓ)=CwΓ1y1=CwΓy1.C_{w_{\Gamma}}\mathbf{P}_{\mathbf{R}}(y^{-1})=C_{w_{\Gamma}}(\mathbf{P}(y))^{\flat}=(\mathbf{P}(y)C_{w_{\Gamma}})^{\flat}=(C_{yw_{\Gamma}})^{\flat}=C_{w_{\Gamma}^{-1}y^{-1}}=C_{w_{\Gamma}y^{-1}}.

The element 𝐏\mathbf{P} in Case (2). Assume that we are in Case (2). We set U={wΓ}U=\{w_{\Gamma}\} and X=XXsX=X^{\prime}\cup X^{\prime}s.

Claim. The set UU together with XX satisfy condition I1I5.

Assume for now that it is the case, then for all yXy\in X we have (note that in the sum below the element xx is chosen in XX and not in XX^{\prime} as above!)

CywΓ\displaystyle C_{yw_{\Gamma}} =TyCwΓ+x<y,xXpxwΓ,ywΓTxCwΓ\displaystyle=T_{y}C_{w_{\Gamma}}+\sum_{x<y,x\in X}p^{*}_{xw_{\Gamma},yw_{\Gamma}}T_{x}C_{w_{\Gamma}}
=(Ty+x<y,xXcpxwΓ,ywΓTz)CwΓ.\displaystyle=\big(T_{y}+\sum_{x<y,x\in X_{c}}p^{*}_{xw_{\Gamma},yw_{\Gamma}}T_{z}\big)C_{w_{\Gamma}}.

For y𝒵1Ty\in\mathcal{Z}^{-1}\cup T we set

𝐏(y)=xy,xXpxwΓ,ywΓTx,𝐏𝐑(y1)=(𝐏(y)),\mathbf{P}(y)=\sum_{x\leq y,x\in X}p^{\ast}_{xw_{\Gamma},yw_{\Gamma}}T_{x},\quad\mathbf{P}_{\mathbf{R}}(y^{-1})=(\mathbf{P}(y))^{\flat},

so that we have

𝐏(y)CwΓ=CywΓ and CwΓ𝐏𝐑(y1)=CwΓy1.\mathbf{P}(y)C_{w_{\Gamma}}=C_{yw_{\Gamma}}\text{ and }C_{w_{\Gamma}}\mathbf{P}_{\mathbf{R}}(y^{-1})=C_{w_{\Gamma}y^{-1}}.

The last equality holds since

CwΓ𝐏𝐑(y1)=CwΓ(𝐏(y))=(𝐏(y)CwΓ)=(CywΓ)=CwΓ1y1=CwΓy1C_{w_{\Gamma}}\mathbf{P}_{\mathbf{R}}(y^{-1})=C_{w_{\Gamma}}(\mathbf{P}(y))^{\flat}=(\mathbf{P}(y)C_{w_{\Gamma}})^{\flat}=(C_{yw_{\Gamma}})^{\flat}=C_{w_{\Gamma}^{-1}y^{-1}}=C_{w_{\Gamma}y^{-1}}

(here we need the fact that wΓ2=1w_{\Gamma}^{2}=1).

Proof of Claim. In order to verify that U={wΓ}U=\{w_{\Gamma}\} together with X=XXsX=X^{\prime}\cup X^{\prime}s satisfies condition I1I5, note that XwΓ=XwXwΓXw_{\Gamma}=X^{\prime}w^{\prime}\cup X^{\prime}w_{\Gamma}, from where conditions I1I3 follow easily. Next we know that {w,wΓ}\{w^{\prime},w_{\Gamma}\} is a left ideal of WW^{\prime}, thus by Corollary 3.10 we get that

𝔅=𝒽Cw|wXwΓXw𝒾𝒜=𝒽CxwΓ|xX𝒾\mathfrak{B}=\mathcal{h}C_{w}\mid w\in X^{\prime}w_{\Gamma}\cup X^{\prime}w^{\prime}\mathcal{i}_{\mathcal{A}}=\mathcal{h}C_{xw_{\Gamma}}\mid x\in X\mathcal{i}

is a left ideal of \mathcal{H}. Since

TxCwΓ=CxwΓ+z<xwΓ,z𝔅Cz,T_{x}C_{w_{\Gamma}}=C_{xw_{\Gamma}}+\sum_{z<xw_{\Gamma},z\in\mathfrak{B}}C_{z},

it follows that 𝔅=𝒽TxCwΓ|xX𝒾\mathfrak{B}=\mathcal{h}T_{x}C_{w_{\Gamma}}\mid x\in X\mathcal{i} and I4 follows. Let xXx\in X. If xXx\in X^{\prime} Condition I5 is clearly satisfied since wΓWw_{\Gamma}\in W^{\prime}. So assume that xXsx\in X^{\prime}s, that is x=xsx=x^{\prime}s for some xXx^{\prime}\in X^{\prime}. Then we have

TxCwΓ\displaystyle T_{x}C_{w_{\Gamma}} =TxTsCwΓ\displaystyle=T_{x^{\prime}}T_{s}C_{w_{\Gamma}}
=Tx(CwvL(s)CwΓ)\displaystyle=T_{x^{\prime}}(C_{w^{\prime}}-v^{-L(s)}C_{w_{\Gamma}})
=TxCwvL(s)TxCwΓ.\displaystyle=T_{x^{\prime}}C_{w^{\prime}}-v^{-L(s)}T_{x^{\prime}}C_{w_{\Gamma}}.

The claim follows since TxCwTxwmod<0T_{x^{\prime}}C_{w^{\prime}}\equiv T_{x^{\prime}w^{\prime}}\mod\mathcal{H}_{<0} and TxCwΓTxwΓmod<0T_{x^{\prime}}C_{w_{\Gamma}}\equiv T_{x^{\prime}w_{\Gamma}}\mod\mathcal{H}_{<0}.

Finally, in both Cases (1) and (2), we set

𝐏(t1mt2n)=𝐏(t1)m𝐏(t2)nif T={t1,t2}𝐏(tn)=𝐏(t)notherwise.\begin{array}[]{rllc}\mathbf{P}(t_{1}^{m}t_{2}^{n})&=\mathbf{P}(t_{1})^{m}\mathbf{P}(t_{2})^{n}&\mbox{if $T=\{t_{1},t_{2}\}$}\\ \mathbf{P}(t^{n})&=\mathbf{P}(t)^{n}&\mbox{otherwise}.\end{array}

4.3. Properties of the element 𝐏\mathbf{P}

Recall that Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} can be viewed as an algebra and that the 𝒜\mathcal{A}-modules

𝒽[Cw]|wΓj𝒾𝒜\mathcal{h}[C_{w}]\mid w\in\Gamma_{j}\mathcal{i}_{\mathcal{A}}

are left ideals in Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} (see Section 3.3).

Lemma 4.2.

Let τ𝒯\tau\in\mathcal{T}. We have

𝐏(τ)CwΓ=CwΓ𝐏R(τ1).\mathbf{P}(\tau)C_{w_{\Gamma}}=C_{w_{\Gamma}}\mathbf{P}_{R}(\tau^{-1}).
Proof.

Using the fact that for all τ𝒯\tau\in\mathcal{T} we have τwΓ=wΓτ1\tau w_{\Gamma}=w_{\Gamma}\tau^{-1} we get

𝐏(τ)CwΓ=CτwΓ=CwΓτ1=CwΓ𝐏R(τ1).\mathbf{P}(\tau)C_{w_{\Gamma}}=C_{\tau w_{\Gamma}}=C_{w_{\Gamma}\tau^{-1}}=C_{w_{\Gamma}}\mathbf{P}_{R}(\tau^{-1}).

We define the following 𝒜\mathcal{A}-submodule of Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma}:

𝒯=𝒽[CτwΓ]|τ𝒯𝒾𝒜.\mathcal{M}_{\mathcal{T}}=\mathcal{h}[C_{\tau w_{\Gamma}}]\mid\tau\in\mathcal{T}\mathcal{i}_{\mathcal{A}}.
Lemma 4.3.

We have

𝒽[Cw]|wΓ1𝒾𝒜𝒽[Cw]|w(Γ1)1𝒾𝒜=𝒯\mathcal{h}[C_{w}]\mid w\in\Gamma_{1}\mathcal{i}_{\mathcal{A}}\cap\mathcal{h}[C_{w}]\mid w\in(\Gamma_{1})^{-1}\mathcal{i}_{\mathcal{A}}=\mathcal{M}_{\mathcal{T}}
Proof.

This follows directly from the fact that 𝒽[Cw]|wΓ1𝒾𝒜\mathcal{h}[C_{w}]\mid w\in\Gamma_{1}\mathcal{i}_{\mathcal{A}} (respectively
𝒽[Cw]|w(Γ1)1𝒾𝒜\mathcal{h}[C_{w}]\mid w\in(\Gamma_{1})^{-1}\mathcal{i}_{\mathcal{A}}) is a left ideal of Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} (respectively a right ideal of Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma}) and the equality

(Γ1)1Γ1={τwΓτ𝒯}.(\Gamma_{1})^{-1}\cap\Gamma_{1}=\{\tau w_{\Gamma}\mid\tau\in\mathcal{T}\}.

Lemma 4.4.

The set {[𝐏(τ)CwΓ]τ𝒯}\{[\mathbf{P}(\tau)C_{w_{\Gamma}}]\mid\tau\in\mathcal{T}\} is an 𝒜\mathcal{A}-basis of 𝒯\mathcal{M}_{\mathcal{T}}.

Proof.

Since 𝐏(τ)CwΓ=CwΓ𝐏R(τ1)\mathbf{P}(\tau)C_{w_{\Gamma}}=C_{w_{\Gamma}}\mathbf{P}_{R}(\tau^{-1}) and

𝐏(τ)CwΓCwΓzwΓ𝒜Cz and CwΓ𝐏R(τ1)CwΓzwΓ𝒜Cz\mathbf{P}(\tau)C_{w_{\Gamma}}\in\mathcal{H}C_{w_{\Gamma}}\subseteq\sum_{z\leq_{\mathcal{L}}w_{\Gamma}}\mathcal{A}C_{z}\text{ and }C_{w_{\Gamma}}\mathbf{P}_{R}(\tau^{-1})\in C_{w_{\Gamma}}\mathcal{H}\subseteq\sum_{z\leq_{\mathcal{R}}w_{\Gamma}}\mathcal{A}C_{z}

we have [𝐏(τ)CwΓ]𝒯[\mathbf{P}(\tau)C_{w_{\Gamma}}]\in\mathcal{M}_{\mathcal{T}} by the previous lemma. Then the result follows easily from the fact that

𝐏(τ)CwΓ=CτwΓ+z<τwΓ𝒜Cz.\mathbf{P}(\tau)C_{w_{\Gamma}}=C_{\tau w_{\Gamma}}+\sum_{z<\tau w_{\Gamma}}\mathcal{A}C_{z}.

Lemma 4.5.

The set {[𝐏(zj1)𝐏(τ)CwΓ]1jm,τ𝒯}\{[\mathbf{P}(z_{j}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}]\mid 1\leq j\leq m,\tau\in\mathcal{T}\} is an 𝒜\mathcal{A}-basis of Γ1\mathcal{M}^{\mathcal{L}}_{\Gamma_{1}}.

Proof.

Since

𝐏(zj1)𝐏(τ)CwΓCwΓzwΓ𝒜Cz\mathbf{P}(z_{j}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\in\mathcal{H}C_{w_{\Gamma}}\subseteq\sum_{z\leq_{\mathcal{L}}w_{\Gamma}}\mathcal{A}C_{z}

we have [𝐏(zj1)𝐏(τ)CwΓ]Γ1[\mathbf{P}(z_{j}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}]\in\mathcal{M}^{\mathcal{L}}_{\Gamma_{1}}. Then the results follows easily from the fact that

𝐏(zj1)𝐏(τ)CwΓ=Czi1τwΓ+z<zi1τwΓCz.\mathbf{P}(z_{j}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}=C_{z_{i}^{-1}\tau w_{\Gamma}}+\sum_{z<z_{i}^{-1}\tau w_{\Gamma}}C_{z}.

4.4. Main result

We are now ready to define the different ingredients needed in order to show that each cell ideal is affine cellular. Recall the definition of TT and 𝒯\mathcal{T} in Section 4.1. As our principal ideal domain kk, we choose 𝒜\mathcal{A}. We set

B={𝒜[t1,t2]if T={t1,t2}𝒜[t]if T={t}𝒜[t]/(t21)if T={e,t}𝒜if T={e}.B=\begin{cases}\mathcal{A}[t_{1},t_{2}]&\mbox{if $T=\{t_{1},t_{2}\}$}\\ \mathcal{A}[t]&\mbox{if $T=\{t\}\qquad$}\\ \mathcal{A}[t]/(t^{2}-1)&\mbox{if $T=\{e,t\}$}\\ \mathcal{A}&\mbox{if $T=\{e\}$.}\end{cases}

Note that the monomials in BB corresponds to the elements of 𝒯\mathcal{T} and we will use this identification freely.
For all 1i,jm1\leq i,j\leq m we know, by Lemma 4.3, that

[CwΓzj][Czi1wΓ]𝒯,[C_{w_{\Gamma}z_{j}}][C_{z_{i}^{-1}w_{\Gamma}}]\in\mathcal{M}_{\mathcal{T}},

thus, by Lemma 4.4, we have

[CwΓzj][Czk1wΓ]=τ𝒯aτj,k[𝐏(τ)CwΓ] where aτj,k𝒜.[C_{w_{\Gamma}z_{j}}][C_{z_{k}^{-1}w_{\Gamma}}]=\sum_{\tau\in\mathcal{T}}a^{j,k}_{\tau}[\mathbf{P}(\tau)C_{w_{\Gamma}}]\text{ where $a^{j,k}_{\tau}\in\mathcal{A}$}.

Let VV be the free 𝒜\mathcal{A}-module of rank mm on basis v1,,vmv_{1},\dots,v_{m} and define the 𝒜\mathcal{A}-bilinear form φ\varphi by

φ:V×VB(vj,vk)τ𝒯aτj,kτ.\begin{array}[]{ccccccc}\varphi:&V\times V&\longrightarrow&B\\ &(v_{j},v_{k})&\longmapsto&\underset{\tau\in\mathcal{T}}{\sum}a^{j,k}_{\tau}\tau.\end{array}

This defines an algebra 𝔸(V,B,φ)V𝒜B𝒜V\mathbb{A}(V,B,\varphi)\cong V\otimes_{\mathcal{A}}B\otimes_{\mathcal{A}}V with multiplication 𝒜\mathcal{A}-bilinearly extended from (viτvj)(vkτvl)=viτφ(vj,vk)τvl(v_{i}\otimes\tau\otimes v_{j})(v_{k}\otimes\tau^{\prime}\otimes v_{l})=v_{i}\otimes\tau\varphi(v_{j},v_{k})\tau^{\prime}\otimes v_{l} as in Section 2.

We now define a map

Φ~:𝔸(V,B,φ)\tilde{\Phi}:\mathbb{A}(V,B,\varphi)\rightarrow\mathcal{H}

by

viτvj𝐏(zi1)𝐏(τ)CwΓ𝐏R(zj)v_{i}\otimes\tau\otimes v_{j}\mapsto\mathbf{P}(z_{i}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})

for basis elements vi,vjv_{i},v_{j} of V and τ𝒯\tau\in\mathcal{T}.

We have

𝐏(zi1)𝐏(τ)CwΓ𝐏R(zj)CwΓzwΓ𝒜Cz.\mathbf{P}(z_{i}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})\in\mathcal{H}C_{w_{\Gamma}}\mathcal{H}\subseteq\sum_{z\leq_{\mathcal{LR}}w_{\Gamma}}\mathcal{A}C_{z}.

Hence, the image of Φ~\tilde{\Phi} is contained in Γ\mathcal{H}_{\leq_{\mathcal{LR}}\Gamma} and we can compose Φ~\tilde{\Phi} with the natural projection [.][\ .\ ] onto Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma}. We obtain a map

Φ:𝔸(V,B,φ)Γviτvj[𝐏(zi1)𝐏(τ)CwΓ𝐏R(zj)].\begin{array}[]{ccccccc}\Phi:&\mathbb{A}(V,B,\varphi)&\longrightarrow&\mathcal{M}^{\mathcal{LR}}_{\Gamma}\\ &v_{i}\otimes\tau\otimes v_{j}&\longmapsto&[\mathbf{P}(z_{i}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})].\end{array}

Note that when B=𝒜[t1,t2]B=\mathcal{A}[t_{1},t_{2}] we have t1mt2n=t2nt1mt_{1}^{m}t_{2}^{n}=t_{2}^{n}t_{1}^{m} in BB thus for Φ\Phi to be well-defined we need to have

Φ(vit1mt2nvj)=Φ(vit2nt1mvj),\Phi(v_{i}\otimes t_{1}^{m}t_{2}^{n}\otimes v_{j})=\Phi(v_{i}\otimes t_{2}^{n}t_{1}^{m}\otimes v_{j}),

that is

[𝐏(zi1)𝐏(t1)m𝐏(t2)nCwΓ𝐏R(zj)]=[𝐏(zi1)𝐏(t2)n𝐏(t1)mCwΓ𝐏R(zj)].[\mathbf{P}(z_{i}^{-1})\mathbf{P}(t_{1})^{m}\mathbf{P}(t_{2})^{n}C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})]=[\mathbf{P}(z_{i}^{-1})\mathbf{P}(t_{2})^{n}\mathbf{P}(t_{1})^{m}C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})].

To prove this, it is enough to show that

[𝐏(t1)𝐏(t2)CwΓ]=[𝐏(t2)𝐏(t1)CwΓ].[\mathbf{P}(t_{1})\mathbf{P}(t_{2})C_{w_{\Gamma}}]=[\mathbf{P}(t_{2})\mathbf{P}(t_{1})C_{w_{\Gamma}}].

This is checked by explicit computation with GAP.

Proposition 4.6.
  1. (1)

    The map Φ:𝔸(V,B,φ)Γ\Phi:\mathbb{A}(V,B,\varphi)\rightarrow\mathcal{M}^{\mathcal{LR}}_{\Gamma} is an isomorphism of 𝒜\mathcal{A}-algebras.

  2. (2)

    Using (1) to define left and right \mathcal{H}-module structures on 𝔸(V,B,φ)\mathbb{A}(V,B,\varphi) by letting hh\in\mathcal{H} act, for v,wVv,w\in V and bBb\in B, as h(vbw)=Φ1(hΦ(vbw)CLOSEh(v\otimes b\otimes w)=\Phi^{-1}(h\Phi(v\otimes b\otimes w) and (vbw)h=Φ1(Φ(vbw)h)(v\otimes b\otimes w)h=\Phi^{-1}(\Phi(v\otimes b\otimes w)h) respectively, Φ\Phi is an isomorphism of \mathcal{H}-\mathcal{H}-bimodules.

  3. (3)

    We have Φ(vbw)=Φ(wbv)\Phi(v\otimes b\otimes w)^{\flat}=\Phi(w\otimes b\otimes v) for v,wVv,w\in V and bBb\in B.

Proof.

The map Φ\Phi is 𝒜\mathcal{A}-linear by definition. We have, for basis elements vi,vj,vk,vlv_{i},v_{j},v_{k},v_{l} of VV and t,t𝒯t,t^{\prime}\in\mathcal{T},

Φ(vitvj)Φ(vktvl)\displaystyle\Phi\big(v_{i}\otimes t\otimes v_{j}\big)\Phi\big(v_{k}\otimes t^{\prime}\otimes v_{l}\big)
=[𝐏(zi1)𝐏(t)CwΓ𝐏R(zj)][𝐏(zk1)𝐏(t)CwΓ𝐏R(zl)]\displaystyle=[\mathbf{P}(z_{i}^{-1})\mathbf{P}(t)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})][\mathbf{P}(z_{k}^{-1})\mathbf{P}(t^{\prime})C_{w_{\Gamma}}\mathbf{P}_{R}(z_{l})]
=[𝐏(zi1)𝐏(t)CwΓzj𝐏(zk1)CwΓ𝐏R(t1)𝐏R(zl)]\displaystyle=[\mathbf{P}(z_{i}^{-1})\mathbf{P}(t)C_{w_{\Gamma}z_{j}}\mathbf{P}(z_{k}^{-1})C_{w_{\Gamma}}\mathbf{P}_{R}(t^{\prime-1})\mathbf{P}_{R}(z_{l})]
=[𝐏(zi1)𝐏(t)CwΓzjCzk1wΓ𝐏R(t1)𝐏R(zl)]\displaystyle=[\mathbf{P}(z_{i}^{-1})\mathbf{P}(t)C_{w_{\Gamma}z_{j}}C_{z_{k}^{-1}w_{\Gamma}}\mathbf{P}_{R}(t^{\prime-1})\mathbf{P}_{R}(z_{l})]
=[𝐏(zi1)𝐏(t)(τ𝒯aτj,k𝐏(τ))CwΓ𝐏R(t1)𝐏R(zl)]\displaystyle=[\mathbf{P}(z_{i}^{-1})\mathbf{P}(t)\big(\sum_{\tau\in\mathcal{T}}a^{j,k}_{\tau}\mathbf{P}(\tau)\big)C_{w_{\Gamma}}\mathbf{P}_{R}(t^{\prime-1})\mathbf{P}_{R}(z_{l})]
=[𝐏(zi1)𝐏(t)(τ𝒯aτj,k𝐏(τ))𝐏(t)CwΓ𝐏R(zl)]\displaystyle=[\mathbf{P}(z_{i}^{-1})\mathbf{P}(t)\big(\sum_{\tau\in\mathcal{T}}a^{j,k}_{\tau}\mathbf{P}(\tau)\big)\mathbf{P}(t^{\prime})C_{w_{\Gamma}}\mathbf{P}_{R}(z_{l})]
=Φ(vitφ(vj,vk)tvl).\displaystyle=\Phi\big(v_{i}\otimes t\varphi(v_{j},v_{k})t^{\prime}\otimes v_{l}\big).

So Φ\Phi is indeed a morphism of 𝒜\mathcal{A}-algebras.

Remark 4.7.

In the case where 𝒯={e,t}\mathcal{T}=\{e,t\} we quotient out by t21t^{2}-1 in BB because we have

(𝐏(t))2CwΓ=CwΓ.(\mathbf{P}(t))^{2}C_{w_{\Gamma}}=C_{w_{\Gamma}}.

The fact that Φ\Phi is bijective follows easily from the fact that

𝐏(zi1)𝐏(τ)CwΓ𝐏R(zj)=Czi1τwΓzj+z<zi1τwΓzj𝒜Cz.\mathbf{P}(z_{i}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})=C_{z_{i}^{-1}\tau w_{\Gamma}z_{j}}+\sum_{z<z_{i}^{-1}\tau w_{\Gamma}z_{j}}\mathcal{A}C_{z}.

This completes the proof of (1).

Claim (2) follows directly from the definition and the fact that Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} is an \mathcal{H}-\mathcal{H}-bimodule.

To prove Claim (3) we let vi,vjv_{i},v_{j} be basis elements of VV and τ𝒯\tau\in\mathcal{T}, and check

Φ(viτvj)\displaystyle\Phi(v_{i}\otimes\tau\otimes v_{j})^{\flat} =[(𝐏(zi1)𝐏(τ)CwΓ𝐏R(zj))]\displaystyle=[(\mathbf{P}(z_{i}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j}))]^{\flat}
=[(𝐏(zi1)𝐏(τ)CwΓ𝐏R(zj))]\displaystyle=[(\mathbf{P}(z_{i}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j}))^{\flat}]
=[(𝐏R(zj))(CwΓ)(𝐏(τ))(𝐏(zi1))]\displaystyle=[(\mathbf{P}_{R}(z_{j}))^{\flat}(C_{w_{\Gamma}})^{\flat}(\mathbf{P}(\tau))^{\flat}(\mathbf{P}(z_{i}^{-1}))^{\flat}]
=[𝐏(zj1)CwΓ𝐏R(τ1)𝐏R(zi)]\displaystyle=[\mathbf{P}(z_{j}^{-1})C_{w_{\Gamma}}\mathbf{P}_{R}(\tau^{-1})\mathbf{P}_{R}(z_{i})]
=[𝐏(zj1)𝐏(τ)CwΓ𝐏R(zi)]\displaystyle=[\mathbf{P}(z_{j}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{i})]
=Φ(vjτvi).\displaystyle=\Phi(v_{j}\otimes\tau\otimes v_{i}).

The claim follows from 𝒜\mathcal{A}-linearity. ∎

Theorem 4.8.

Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} is an affine cell ideal in /<Γ\mathcal{H}/\mathcal{H}_{<_{\mathcal{LR}}\Gamma} with the 𝒜\mathcal{A}-involution induced by \flat.

Proof.

According to Proposition 2.2, this follows from Proposition 4.6 by choosing the 𝒜\mathcal{A}-involution on BB to be the identity. ∎

4.5. Remaining cases

Assume that WW is of type G~2\tilde{G}_{2} (as in Example 3.6) and that Γ\Gamma be a finite two-sided cell which intersect the group generated by s2,s3s_{2},s_{3}. Let

Γ=i=1mΓi\Gamma=\bigcup_{i=1}^{m}\Gamma_{i}

be the decomposition of Γ\Gamma into left cells.

Assume that a>ba>b. Then it can be checked by inspection that for all i,ji,j we have that (Γi)1Γj(\Gamma_{i})^{-1}\cap\Gamma_{j} only contains one element: we will denote it by wi,jw^{i,j}.

Note that this implies that each left cell contains mm elements. Let VV be a mm-dimensional 𝒜\mathcal{A}-module on basis v1,,vmv_{1},\dots,v_{m} and let B=𝒜B=\mathcal{A}. Let

φ:V×VB(vj,vk)aj,k\begin{array}[]{ccccccc}\varphi:&V\times V&\longrightarrow&B\\ &(v_{j},v_{k})&\longmapsto&a_{j,k}\end{array}

where aj,kBa_{j,k}\in B is such that

[Cw1,j][Cwk,1]=aj,k[Cw1,1].[C_{w^{1,j}}][C_{w^{k,1}}]=a_{j,k}[C_{w^{1,1}}].

Then it can be checked in each case that the map

Φ:𝔸(V,B,φ)Γvi1vj[Cwi,j]\begin{array}[]{ccccccc}\Phi:&\mathbb{A}(V,B,\varphi)&\longrightarrow&\mathcal{M}^{\mathcal{LR}}_{\Gamma}\\ &v_{i}\otimes 1\otimes v_{j}&\longmapsto&[C_{w^{i,j}}]\end{array}

satisfies the required properties. This is proved by explicit computation.

Assume that a<ba<b. Then Γ=Γ1Γ2Γ3\Gamma=\Gamma_{1}\cup\Gamma_{2}\cup\Gamma_{3} where

Γ1\displaystyle\Gamma_{1} ={s3,s2s3,s1s2s3,s2s1s2s3,s3s2s1s2s3,s1s2s1s2s3},\displaystyle=\{s_{3},s_{2}s_{3},s_{1}s_{2}s_{3},s_{2}s_{1}s_{2}s_{3},s_{3}s_{2}s_{1}s_{2}s_{3},s_{1}s_{2}s_{1}s_{2}s_{3}\},
Γ2\displaystyle\Gamma_{2} ={s2,s3s2,s1s2,s2s1s2,s3s2s1s2,s1s2s1s2},\displaystyle=\{s_{2},s_{3}s_{2},s_{1}s_{2},s_{2}s_{1}s_{2},s_{3}s_{2}s_{1}s_{2},s_{1}s_{2}s_{1}s_{2}\},
Γ3\displaystyle\Gamma_{3} ={s2s1,s3s2s1,s1s2s1,s2s1s2s1,s3s2s1s2s1,s1s2s1s2s1}.\displaystyle=\{s_{2}s_{1},s_{3}s_{2}s_{1},s_{1}s_{2}s_{1},s_{2}s_{1}s_{2}s_{1},s_{3}s_{2}s_{1}s_{2}s_{1},s_{1}s_{2}s_{1}s_{2}s_{1}\}.

Let B=𝒜[t]/(t21)B=\mathcal{A}[t]/(t^{2}-1) and let VV be a 3-dimensional 𝒜\mathcal{A}-module with basis E:={v1,v2,v3}E:=\{v_{1},v_{2},v_{3}\}. Let

ϕ:E×{1,t}×EΓ\phi:E\times\{1,t\}\times E\rightarrow\Gamma

be such that ϕ(vi,1,vj)\phi(v_{i},1,v_{j}) (respectively ϕ(vi,t,vj)\phi(v_{i},t,v_{j})) is the element of minimal (respectively of maximal) length in (Γi)1Γj(\Gamma_{i})^{-1}\cap\Gamma_{j}. Then we define φ:V×VB\varphi:V\times V\rightarrow B by the following matrix

(a1a2+t1a2+ta3+a4t010a1)\left(\begin{array}[]{ccc}a_{1}&a_{2}+t&1\\ a_{2}+t&a_{3}+a_{4}t&0\\ 1&0&a_{1}\end{array}\right)

where

a1=vb+vba2=vab+vbaa3=vb+v2ab+vb2a+vba4=va+va.\begin{array}[]{llllll}a_{1}&=v^{b}+v^{-b}&a_{2}&=v^{a-b}+v^{b-a}\\ a_{3}&=v^{-b}+v^{2a-b}+v^{b-2a}+v^{b}&a_{4}&=v^{-a}+v^{a}.\end{array}

Finally we set

Φ:𝔸(V,B,φ)Γvi1vj[Cϕ(vi,1,vj)]vitvj[Cϕ(vi,t,vj)].\begin{array}[]{ccccccc}\Phi:&\mathbb{A}(V,B,\varphi)&\longrightarrow&\mathcal{M}^{\mathcal{LR}}_{\Gamma}\\ &v_{i}\otimes 1\otimes v_{j}&\longmapsto&[C_{\phi(v_{i},1,v_{j})}]\\ &v_{i}\otimes t\otimes v_{j}&\longmapsto&[C_{\phi(v_{i},t,v_{j})}].\end{array}

Then it can be checked by explicit computations that Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} is affine cellular in the quotient /<Γ\mathcal{H}/\mathcal{H}_{<_{\mathcal{LR}}\Gamma}.

4.6. Proof of Theorem 1.1

Theorem 1.1 now follows from the results in Subsections 4.4 and 4.5. Indeed, let WW be an affine Weyl group of rank 2 together with a generic weight function LL and let \mathcal{H} be the associated Hecke algebra. Consider the filtration of \mathcal{H} by two-sided ideals Γ\mathcal{H}_{\leq_{\mathcal{LR}}\Gamma} given by the partial order \leq_{\mathcal{LR}} on two-sided cells Γ\Gamma of WW. We need to show that the Kazhdan-Lusztig cell modules Γ\mathcal{M}_{\Gamma}^{\mathcal{LR}} are isomorphic to some 𝔸(V,B,φ)\mathbb{A}(V,B,\varphi). First we show that “most” of the two-sided cells Γ\Gamma of WW can be described as

Γ={z1τwΓzτ𝒯,z,z𝒵}\Gamma=\{z^{-1}\tau w_{\Gamma}z^{\prime}\mid\tau\in\mathcal{T},z,z^{\prime}\in\mathcal{Z}\}

for some subsets 𝒯,𝒵\mathcal{T},\mathcal{Z} of WW and wΓWw_{\Gamma}\in W (see Sections 4.1, Section 5 and Appendix A). Then, using the Generalised Induction Theorem of Kazhdan-Lusztig cells (see Section 3.6), we define polynomials 𝐏(τ)𝒜\mathbf{P}(\tau)\in\mathcal{A} for all τ𝒯\tau\in\mathcal{T} (see Section 4.2). Finally, we show that the map

Φ:𝔸(V,B,φ)Γviτvj[𝐏(zi1)𝐏(τ)CwΓ𝐏R(zj)]\begin{array}[]{ccccccc}\Phi:&\mathbb{A}(V,B,\varphi)&\longrightarrow&\mathcal{M}^{\mathcal{LR}}_{\Gamma}\\ &v_{i}\otimes\tau\otimes v_{j}&\longmapsto&[\mathbf{P}(z_{i}^{-1})\mathbf{P}(\tau)C_{w_{\Gamma}}\mathbf{P}_{R}(z_{j})]\end{array}

is an isomorphism of 𝒜\mathcal{A}-algebras (see Section 4.4). We then treat the case of the two-sided cells which cannot be described as above in Section 4.5.

Applying the results in Section 2, we obtain a parameterisation of simple modules of \mathcal{H}: For each cell we obtain a simple module for every maximal ideal of the corresponding 𝒜\mathcal{A}-algebra BB, defined at the start of Subsection 4.4. If we specialise to (v)𝒜\mathbb{C}(v)\otimes_{\mathcal{A}}\mathcal{H}, the parametrisation is simply given by tuples (a,b)(v)2(a,b)\in\mathbb{C}(v)^{2} if T={t1,t2}T=\{t_{1},t_{2}\}, a(v)a\in\mathbb{C}(v) if T={t}T=\{t\}, ±1\pm 1 if T={e,t}T=\{e,t\}, and 11 if T={e}T=\{e\}. Also it is clear that the affine 𝒜\mathcal{A}-algebras BB that appear in our construction satisfy rad(B)=0\mathrm{rad}(B)=0 and have finite global dimension. Thus in order to prove that the affine Hecke algebra \mathcal{H} has finite global dimension, using the affine cellular structure, one would need to show that every Γ\mathcal{M}^{\mathcal{LR}}_{\Gamma} is an idempotent ideal in /<Γ\mathcal{H}/\mathcal{H}_{<_{\mathcal{LR}}\Gamma} and that it contains an idempotent element in /<Γ\mathcal{H}/\mathcal{H}_{<_{\mathcal{LR}}\Gamma}.

Remark 4.9.

The problem of finiteness of global dimension of affine Hecke algebras have already been addressed by Opdam and Solleveld in [12]. Using methods of harmonic analysis, they determined the (finite) global dimension of affine Hecke algebras in the case where vv is specialized to a positive real number.

5. Examples

The aim of this section is to provide some explicit examples of the sets 𝒵\mathcal{Z} and 𝒯\mathcal{T} as defined in Section 4.1. Let WW be an affine Weyl group of type G~2\tilde{G}_{2} as in Example 3.6 together with some generic parameters a,ba,b such that a/b>2a/b>2. The partition into cells in this case is shown in the following figure: the left cells are formed by the alcoves lying in the same connected component after removing the thick lines and the two-sided cells are the unions of all the left cells whose names share the same subscript. The alcove corresponding to the identity is denoted by c~61\tilde{c}_{6}^{1}. We use the geometric presentation of WW as defined in [10].

-6,-6.4)(6,6.4)

We first have a look at the lowest two-sided cell c~0\tilde{c}_{0}. In Figure 1, we show the elements of the set 𝒵={z1,,z12}\mathcal{Z}=\{z_{1},\ldots,z_{12}\}: these are the elements which correspond to the alcoves in dark gray. The alcoves lying in the box in light gray correspond to the elements in 𝒵1\mathcal{Z}^{-1}. We set t1=s2s1s2s1s2s3t_{1}=s_{2}s_{1}s_{2}s_{1}s_{2}s_{3}, t2=s1s2s1s2s3s1s2s1s2s3t_{2}=s_{1}s_{2}s_{1}s_{2}s_{3}s_{1}s_{2}s_{1}s_{2}s_{3} and

𝒯:={t1nt2m|n,m}.\mathcal{T}:=\{t_{1}^{n}t_{2}^{m}|n,m\in\mathbb{N}\}.

Then we have

c~0\displaystyle\tilde{c}_{0} ={zi1τw0zjτ𝒯,1i,j12}\displaystyle=\{z_{i}^{-1}\tau w_{0}z_{j}\mid\tau\in\mathcal{T},1\leq i,j\leq 12\}
c~0j\displaystyle\tilde{c}_{0}^{j} ={zi1τw0zjτ𝒯,1j12}.\displaystyle=\{z_{i}^{-1}\tau w_{0}z_{j}\mid\tau\in\mathcal{T},1\leq j\leq 12\}.

where w0=w1,2w_{0}=w_{1,2}. This should be understood in the following way. Let w=zi1τw0zjc~0w=z_{i}^{-1}\tau w_{0}z_{j}\in\tilde{c}_{0}. The element zjz_{j} indicate in which connected component of c~0\tilde{c}_{0} the element ww lies. Then τ\tau indicates in which translate of the box ww lies and finally zi1z_{i}^{-1} indicates where in the translate of box ww lies. This is explained in Figure 1.

Figure 1. Description of c~0\tilde{c}_{0}


We now have a look at the two-sided cell c~1\tilde{c}_{1}. We set w1=s1s2s1s2s1w_{1}=s_{1}s_{2}s_{1}s_{2}s_{1}. In Figure 2, we show the elements of the set 𝒵={z1,,z6}\mathcal{Z}=\{z_{1},\ldots,z_{6}\}: these are the elements which correspond to the alcoves in dark gray. We set t=s1s2s1s2s3t=s_{1}s_{2}s_{1}s_{2}s_{3} and

𝒯:={tn|n}.\mathcal{T}:=\{t^{n}|n\in\mathbb{N}\}.

Then we have

c~1\displaystyle\tilde{c}_{1} ={zi1τw1zjτ𝒯,1i,j6}\displaystyle=\{z_{i}^{-1}\tau w_{1}z_{j}\mid\tau\in\mathcal{T},1\leq i,j\leq 6\}
c~1j\displaystyle\tilde{c}_{1}^{j} ={zi1τw1zjτ𝒯,1j6}.\displaystyle=\{z_{i}^{-1}\tau w_{1}z_{j}\mid\tau\in\mathcal{T},1\leq j\leq 6\}.

This is explained in Figure 2.

Figure 2. Description of the two-sided cell c~1\tilde{c}_{1}


We now have a look at the two-sided cell c~2\tilde{c}_{2}. We set w2=s1s3w_{2}=s_{1}s_{3}. In Figure 3, we show the elements of the set 𝒵={z1,,z6}\mathcal{Z}=\{z_{1},\ldots,z_{6}\}: these are the elements which correspond to the alcoves in dark gray. We set t=s1s3s2t=s_{1}s_{3}s_{2} and

𝒯:={tn|n}.\mathcal{T}:=\{t^{n}|n\in\mathbb{N}\}.

Then we have

c~2\displaystyle\tilde{c}_{2} ={zi1τw2zjτ𝒯,1i,j6}\displaystyle=\{z_{i}^{-1}\tau w_{2}z_{j}\mid\tau\in\mathcal{T},1\leq i,j\leq 6\}
c~2j\displaystyle\tilde{c}_{2}^{j} ={zi1τw2zjτ𝒯,1j6}.\displaystyle=\{z_{i}^{-1}\tau w_{2}z_{j}\mid\tau\in\mathcal{T},1\leq j\leq 6\}.

This is explained in Figure 3.

Figure 3. Description of the two-sided cell c~2\tilde{c}_{2}

We now have a look at c~3\tilde{c}_{3}. We set wc~3=s1w_{\tilde{c}_{3}}=s_{1}, 𝒵={z1,z2,z3}={e,s2,s2s3}\mathcal{Z}=\{z_{1},z_{2},z_{3}\}=\{e,s_{2},s_{2}s_{3}\} and

𝒯:={e,s1s2}.\mathcal{T}:=\{e,s_{1}s_{2}\}.

Then we have

c~3\displaystyle\tilde{c}_{3} ={zi1τw1zjτ𝒯,1i,j3}\displaystyle=\{z_{i}^{-1}\tau w_{1}z_{j}\mid\tau\in\mathcal{T},1\leq i,j\leq 3\}
c~3j\displaystyle\tilde{c}_{3}^{j} ={zi1τw1zjτ𝒯,1j3}.\displaystyle=\{z_{i}^{-1}\tau w_{1}z_{j}\mid\tau\in\mathcal{T},1\leq j\leq 3\}.

Finally, we have a look at c~4={s2s3s2}\tilde{c}_{4}=\{s_{2}s_{3}s_{2}\}. In this case, if we set wc~4=s2s3s2w_{\tilde{c}_{4}}=s_{2}s_{3}s_{2} and 𝒵=𝒯={e}\mathcal{Z}=\mathcal{T}=\{e\}, the description in Section 4.1 clearly holds.

Appendix A Some additional data

The aim of this Appendix is to gather some data about cells in affine Weyl groups of rank 2 which are needed in the proof of Proposition 4.6. We refer to [6] and [8] for details.

In this appendix, (W,S)(W,S) will denote an affine Weyl group of type GG or BB together with a generic weight function LL. We set

=ISWI.\mathfrak{C}=\bigcup_{I\subsetneq S}W_{I}.

Let x,yx,y\in\mathfrak{C}; we write x,yx\sim_{\mathcal{L}\mathcal{R},\mathfrak{C}}y if there exist a sequence x=x0,,xn=yx=x_{0},...,x_{n}=y in \mathfrak{C} and a sequence I0,,In1I_{0},...,I_{n-1} of subsets of SS such that

xk,xk+1WIkx_{k},x_{k+1}\in W_{I_{k}} and xkxk+1x_{k}\sim_{\mathcal{LR}}x_{k+1} in WIkW_{I_{k}}

for all 0kn10\leq k\leq n-1. This an equivalence relation and the equivalence classes will be called (for obvious reasons) the two-sided cells of \mathfrak{C}. We denote by 𝒫,\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}} the associated partition of \mathfrak{C}. It can be shown that the Lusztig 𝐚\mathbf{a}-function is constant on each of the equivalence classes. To each c𝒫,c\in\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}}, starting from the one with highest 𝐚\mathbf{a}-value, we associate the following subset of WW:

c~={wW|w=xuy,(w)=(x)+(u)+(y),x,yW,uc}𝐚(c)>𝐚(c)c~.\tilde{c}=\{w\in W\ |\ w=xuy,\ell(w)=\ell(x)+\ell(u)+\ell(y),\ x,y\in W,u\in c\}-\bigcup_{\mathbf{a}(c^{\prime})>\mathbf{a}(c)}\tilde{c}^{\prime}.

Then the sets c~\tilde{c} are the two-sided cells of WW with respect to LL and the left cells lying in c~\tilde{c} are the connected component of c~\tilde{c}.

Remark A.1.

In [8], we introduced another equivalence relation denoted \sim_{\mathfrak{C}}. In our case, since the weight function is generic, it can be shown that the two equivalence relations ,\sim_{\mathcal{L}\mathcal{R},\mathfrak{C}} and \sim_{\mathfrak{C}} are the same.

For each choice of parameters, we give the following data:

  1. (1)

    the partition 𝒫,\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}};

  2. (2)

    an ordering of 𝒫,\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}} with respect to Lusztig 𝐚\mathbf{a}-function.

These data determine the partition of WW into cells. The explicit partition can be found in [8] in type GG and in [6] in type BB.

Remark A.2.

We sometime write cicjc_{i}\leftrightarrow c_{j} in the ordering of 𝒫,\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}} to signify that for some values of the parameters we have 𝐚(ci)>𝐚(cj)\mathbf{a}(c_{i})>\mathbf{a}(c_{j}) and for some others we have 𝐚(cj)𝐚(ci)\mathbf{a}(c_{j})\geq\mathbf{a}(c_{i}) but the corresponding sets c~i\tilde{c}_{i} and c~j\tilde{c}_{j} are the same whether c~i\tilde{c}_{i} or c~j\tilde{c}_{j} is computed first in the process.

Let c~\tilde{c} be a two-sided cell associated to c𝒫,c\in\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}} with left cells decomposition

c~:=c~i (i=1m).\tilde{c}:=\bigcup\tilde{c}^{i}\text{ ($i=1\ldots m$)}.

We define an element wcWw_{c}\in W and two subsets 𝒵:={z1,,zm}\mathcal{Z}:=\{z_{1},\ldots,z_{m}\} and 𝒯\mathcal{T} such that

c~={zi1τwczjτ𝒯,1i,jm},c~j={zi1τwczjτ𝒯,1im},(c~i)1c~j={zi1τwczjτ𝒯}.\begin{array}[]{rcl}\tilde{c}&=&\{z_{i}^{-1}\tau w_{c}z_{j}\mid\tau\in\mathcal{T},1\leq i,j\leq m\},\\ \tilde{c}^{j}&=&\{z_{i}^{-1}\tau w_{c}z_{j}\mid\tau\in\mathcal{T},1\leq i\leq m\},\\ (\tilde{c}^{i})^{-1}\cap\tilde{c}^{j}&=&\{z_{i}^{-1}\tau w_{c}z_{j}\mid\tau\in\mathcal{T}\}.\end{array}

We introduce the following notation for tWt\in W:

𝒽t𝒾\displaystyle\mathcal{h}t\mathcal{i} ={tnn},\displaystyle=\{t^{n}\mid n\in\mathbb{N}\},
t^\displaystyle\widehat{t} ={wW(w1t)=(t)(w)}.\displaystyle=\{w\in W\mid\ell(w^{-1}t)=\ell(t)-\ell(w)\}.
Remark A.3.

In other word the set t^\hat{t} consists of all the elements s1sks_{1}\ldots s_{k} where k(t)k\leq\ell(t) such that there exists a reduced expression of tt of the form s1sksk+1s(t)s_{1}\ldots s_{k}s_{k+1}\ldots s_{\ell(t)}. For instance

s1s2s3^={e,s1,s1s2,s1s2s3} and s1s3^={e,s1,s3,s1s3}\widehat{s_{1}s_{2}s_{3}}=\{e,s_{1},s_{1}s_{2},s_{1}s_{2}s_{3}\}\text{ and }\widehat{s_{1}s_{3}}=\{e,s_{1},s_{3},s_{1}s_{3}\}

A.1. Affine Weyl group of type GG

We keep the setting of Example 3.6. As far as the lowest two-sided cell c~0\tilde{c}_{0} is concerned, the sets 𝒯,𝒵\mathcal{T},\mathcal{Z} and the element wc0w_{c_{0}} are the same as in Section 5 for all choices of parameters.

Case 𝐫>𝟏{\bf r>1}.

Table 1. Partition 𝒫,\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}} and values of the 𝐚\mathbf{a}-function

c6={e}0c5=W2,3{w2,3,e}bc4={w2,3}3bc3=W1,2{e,s2,s1s2s1s2s1,w1,2}ac2={w1,3}a+bc1={s1s2s1s2s1}3a2bc0={w1,2}3a+3b\begin{array}[]{|l|c|}\hline\cr c_{6}=\{e\}&0\\ c_{5}=W_{2,3}-\{w_{2,3},e\}&b\\ c_{4}=\{w_{2,3}\}&3b\\ c_{3}=W_{1,2}-\{e,s_{2},s_{1}s_{2}s_{1}s_{2}s_{1},w_{1,2}\}&a\\ c_{2}=\{w_{1,3}\}&a+b\\ c_{1}=\{s_{1}s_{2}s_{1}s_{2}s_{1}\}&3a-2b\\ c_{0}=\{w_{1,2}\}&3a+3b\\ \hline\cr\end{array}

Table 2. Ordering of the partition 𝒫\mathcal{P}_{\mathfrak{C}}

r>2c0c1c2c3c4c5c62>r>3/2c0c1c4c2c3c5c63/2>r>1c0c4c2c1c3c5c6\begin{array}[]{|c|ccccccc|}\hline\cr r>2&c_{0}&c_{1}&c_{2}&\lx@intercol c_{3}\overset{}{\leftrightarrow}c_{4}\hfil\lx@intercol&c_{5}&c_{6}\\ \hline\cr 2>r>3/2&c_{0}&\lx@intercol\hfil c_{1}\overset{}{\leftrightarrow}c_{4}\hfil\lx@intercol&c_{2}&c_{3}&c_{5}&c_{6}\\ \hline\cr 3/2>r>1&c_{0}&c_{4}&c_{2}&c_{1}&c_{3}&c_{5}&c_{6}\\ \hline\cr\end{array}

Table 3. The sets 𝒯\mathcal{T} and 𝒵\mathcal{Z}

r>22>r>3/23/2>r>1wcic~1,𝒯𝒽s1s2s1s2s3𝒾𝒽s2s2s1s2s3𝒾{e}s1s2s1s2s1𝒵s3s2s1s2s3^s3s2s1s2s3^{e}c~2,𝒯𝒽s1s3s2𝒾{e}𝒽s1s3s2s1s2𝒾s1s3𝒵s2s1s2s3^{s2s3}s2s1s2s3^s2s1s2s1^{s2s1s2s3}c~3,𝒯{e,s1s2}{e,s1s2}{e,s1s2}s1𝒵s2s3^s2s3^s2s3^c~4,𝒯{e}𝒽s3s2s1𝒾𝒽s3s2s1𝒾s2s3s2𝒵{e}s1s2s1s2s3^s1s2s1s2s3^\begin{array}[]{|cc|c|c|c|c|}\hline\cr&&r>2&2>r>3/2&3/2>r>1&w_{c_{i}}\\ \hline\cr\tilde{c}_{1},&\mathcal{T}&\mathcal{h}s_{1}s_{2}s_{1}s_{2}s_{3}\mathcal{i}&\mathcal{h}s_{2}s_{2}s_{1}s_{2}s_{3}\mathcal{i}&\{e\}&s_{1}s_{2}s_{1}s_{2}s_{1}\\ &\mathcal{Z}&\widehat{s_{3}s_{2}s_{1}s_{2}s_{3}}&\widehat{s_{3}s_{2}s_{1}s_{2}s_{3}}&\{e\}&\\ \hline\cr\tilde{c}_{2},&\mathcal{T}&\mathcal{h}s_{1}s_{3}s_{2}\mathcal{i}&\{e\}&\mathcal{h}s_{1}s_{3}s_{2}s_{1}s_{2}\mathcal{i}&s_{1}s_{3}\\ &\mathcal{Z}&\widehat{s_{2}s_{1}s_{2}s_{3}}\cup\{s_{2}s_{3}\}&\widehat{s_{2}s_{1}s_{2}s_{3}}&\widehat{s_{2}s_{1}s_{2}s_{1}}\cup\{s_{2}s_{1}s_{2}s_{3}\}&\\ \hline\cr\tilde{c}_{3},&\mathcal{T}&\{e,s_{1}s_{2}\}&\{e,s_{1}s_{2}\}&\{e,s_{1}s_{2}\}&s_{1}\\ &\mathcal{Z}&\widehat{s_{2}s_{3}}&\widehat{s_{2}s_{3}}&\widehat{s_{2}s_{3}}&\\ \hline\cr\tilde{c}_{4},&\mathcal{T}&\{e\}&\mathcal{h}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{3}s_{2}s_{1}\mathcal{i}&s_{2}s_{3}s_{2}\\ &\mathcal{Z}&\{e\}&\widehat{s_{1}s_{2}s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{1}s_{2}s_{3}}&\\ \hline\cr\end{array}

Case 𝐫<𝟏{\bf r<1}.

Table 4. Partition 𝒫,\mathcal{P}_{\mathcal{L}\mathcal{R},\mathfrak{C}} and value of the 𝐚\mathbf{a}-function when b>ab>a

c6={e}0c5={s1}ac4={e,s1,s2s1s2s1s2,w1,2,w1,3,w2,3}bc3={w1,3}a+bc2={s2s1s2s1s2}3b2ac1={w2,3}3bc0={w1,2}3a+3b\begin{array}[]{|l|c|}\hline\cr c_{6}=\{e\}&0\\ c_{5}=\{s_{1}\}&a\\ c_{4}=\mathfrak{C}-\{e,s_{1},s_{2}s_{1}s_{2}s_{1}s_{2},w_{1,2},w_{1,3},w_{2,3}\}&b\\ c_{3}=\{w_{1,3}\}&a+b\\ c_{2}=\{s_{2}s_{1}s_{2}s_{1}s_{2}\}&3b-2a\\ c_{1}=\{w_{2,3}\}&3b\\ c_{0}=\{w_{1,2}\}&3a+3b\\ \hline\cr\end{array}

We get the following ordering

c0c1c2c3c4c5c6.c_{0}\ c_{1}\ c_{2}\leftrightarrow c_{3}\ c_{4}\ c_{5}\ c_{6}.
Table 5. The sets 𝒯\mathcal{T} and 𝒵\mathcal{Z}

r<1wcic~1,𝒯𝒽s3s2s1𝒾s2s3s2𝒵s1s2s1s2s3^c~2,𝒯{e}s2s1s2s1s2𝒵s3^c~3,𝒯𝒽s1s3s2s1s2𝒾s1s3𝒵s2s1s2s1^{s2s1s2s3}c~5,𝒯{e}s1𝒵{e}\begin{array}[]{|cc|c|c|c|}\hline\cr&&r<1&w_{c_{i}}\\ \hline\cr\tilde{c}_{1},&\mathcal{T}&\mathcal{h}s_{3}s_{2}s_{1}\mathcal{i}&s_{2}s_{3}s_{2}\\ &\mathcal{Z}&\widehat{s_{1}s_{2}s_{1}s_{2}s_{3}}&\\ \hline\cr\tilde{c}_{2},&\mathcal{T}&\{e\}&s_{2}s_{1}s_{2}s_{1}s_{2}\\ &\mathcal{Z}&\widehat{s_{3}}&\\ \hline\cr\tilde{c}_{3},&\mathcal{T}&\mathcal{h}s_{1}s_{3}s_{2}s_{1}s_{2}\mathcal{i}&s_{1}s_{3}\\ &\mathcal{Z}&\widehat{s_{2}s_{1}s_{2}s_{1}}\cup\{s_{2}s_{1}s_{2}s_{3}\}&\\ \hline\cr\tilde{c}_{5},&\mathcal{T}&\{e\}&s_{1}\\ &\mathcal{Z}&\{e\}&\\ \hline\cr\end{array}


A.2. Affine Weyl group of type BB

We keep the setting of Example 3.7. As far as the lowest two-sided cell c~0\tilde{c}_{0} is concerned, the set 𝒯\mathcal{T}, 𝒵\mathcal{Z} and the element wc0w_{c_{0}} are the same for all choices of parameters, namely wc0=s1s2s1s2w_{c_{0}}=s_{1}s_{2}s_{1}s_{2},

𝒵=s3s2s1s3s2s3^\mathcal{Z}=\widehat{s_{3}s_{2}s_{1}s_{3}s_{2}s_{3}}

and

𝒯={t1mt2nn,m}\mathcal{T}=\{t_{1}^{m}t_{2}^{n}\mid n,m\in\mathbb{N}\}

where t1=s2s1s2s3t_{1}=s_{2}s_{1}s_{2}s_{3}, t2=s1s2s1s3s2s3t_{2}=s_{1}s_{2}s_{1}s_{3}s_{2}s_{3}.

Generic parameters in zone AiA_{i} (1i51\leq i\leq 5).

Table 6. Partition 𝒫LR,\mathcal{P}_{LR,\mathfrak{C}} and values of the 𝐚\mathbf{a}-function

c8={e}0c7={s3}cc6={s2,s3s2,s2s3,s3s2s3}bc5={s2s3s2}2bcc4={s2s3s2s3}2b+2cc3={s1,s2s1,s1s2,s2s1s2}ac2={s1s3}a+cc1={s1s2s1}2abc0={w1,2}2a+2b\begin{array}[]{|l|c|}\hline\cr c_{8}=\{e\}&0\\ c_{7}=\{s_{3}\}&c\\ c_{6}=\{s_{2},s_{3}s_{2},s_{2}s_{3},s_{3}s_{2}s_{3}\}&b\\ c_{5}=\{s_{2}s_{3}s_{2}\}&2b-c\\ c_{4}=\{s_{2}s_{3}s_{2}s_{3}\}&2b+2c\\ c_{3}=\{s_{1},s_{2}s_{1},s_{1}s_{2},s_{2}s_{1}s_{2}\}&a\\ c_{2}=\{s_{1}s_{3}\}&a+c\\ c_{1}=\{s_{1}s_{2}s_{1}\}&2a-b\\ c_{0}=\{w_{1,2}\}&2a+2b\\ \hline\cr\end{array}

Table 7. Partition 𝒫\mathcal{P}_{\mathfrak{C}}

(r1,r2)A1c0c1c2c3c4c5c6c7c8(r1,r2)A2c0c1c4c2c3c5c6c7c8(r1,r2)A3c0c1c4c2c5c3c6c7c8(r1,r2)A4c0c4c2c1c5c3c6c7c8(r1,r2)A5c0c4c2c1c3c5c6c7c8\begin{array}[]{|c|ccccccccc|}\hline\cr(r_{1},r_{2})\in A_{1}&c_{0}&c_{1}&c_{2}&\lx@intercol\hfil c_{3}\leftrightarrow c_{4}\lx@intercol&c_{5}&c_{6}&c_{7}&c_{8}\\ \hline\cr(r_{1},r_{2})\in A_{2}&c_{0}&c_{1}&c_{4}&c_{2}&c_{3}&c_{5}&c_{6}&c_{7}&c_{8}\\ \hline\cr(r_{1},r_{2})\in A_{3}&c_{0}&\lx@intercol\hfil c_{1}\leftrightarrow c_{4}\lx@intercol&c_{2}&c_{5}&c_{3}&c_{6}&c_{7}&c_{8}\\ \hline\cr(r_{1},r_{2})\in A_{4}&c_{0}&c_{4}&c_{2}&c_{1}&c_{5}&c_{3}&c_{6}&c_{7}&c_{8}\\ \hline\cr(r_{1},r_{2})\in A_{5}&c_{0}&c_{4}&c_{2}&c_{1}&c_{3}&c_{5}&c_{6}&c_{7}&c_{8}\\ \hline\cr\end{array}

Table 8. The sets 𝒵\mathcal{Z} and 𝒯\mathcal{T}

A1A2A3A4A5wcic~1,𝒯𝒽s1s2s3𝒾𝒽s1s2s3𝒾𝒽s1s2s3𝒾{e}{e}s1s2s1𝒵s3s2s3^s3s2s3^s3s2s3^{e}{e}c~2,𝒯𝒽s1s2s3s2𝒾{e}{e}𝒽s1s3s2𝒾𝒽s1s3s2𝒾s1s3𝒵s2s3s2^s2s3^s2s3^s2s1^{s2s3}s2s1^{s2s3}c~3,𝒯𝒽s1s2s3s2𝒾𝒽s1s2s3s2𝒾{e}{e}𝒽s1s2s3s2𝒾s1𝒵s2s3s2^s2s3s2^s2s3^s2s3^s2s3s2^c~4,𝒯{e}𝒽s2s3s2s1𝒾𝒽s2s3s2s1𝒾𝒽s2s3s2s1𝒾𝒽s2s3s2s1𝒾s2s3s2s3𝒵{e}s1s2s3^s1s2s3^s1s2s3^s1s2s3^c~5,𝒯{e}{e}𝒽s2s3s2s1𝒾𝒽s2s3s2s1𝒾{e}s2s3s2𝒵{e}{e}s1s2s3^s1s2s3^{e}c~6,𝒯{e}{e}{e}{e}{e}s2𝒵s3^s3^s3^s3^s3^c~7,𝒯{e}{e}{e}{e}{e}s3𝒵{e}{e}{e}{e}{e}\begin{array}[]{|cc|c|c|c|c|c|c|}\hline\cr&&A_{1}&A_{2}&A_{3}&A_{4}&A_{5}&w_{c_{i}}\\ \hline\cr\tilde{c}_{1},&\mathcal{T}&\mathcal{h}s_{1}s_{2}s_{3}\mathcal{i}&\mathcal{h}s_{1}s_{2}s_{3}\mathcal{i}&\mathcal{h}s_{1}s_{2}s_{3}\mathcal{i}&\{e\}&\{e\}&s_{1}s_{2}s_{1}\\ &\mathcal{Z}&\widehat{s_{3}s_{2}s_{3}}&\widehat{s_{3}s_{2}s_{3}}&\widehat{s_{3}s_{2}s_{3}}&\{e\}&\{e\}&\\ \hline\cr\tilde{c}_{2},&\mathcal{T}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&\{e\}&\{e\}&\mathcal{h}s_{1}s_{3}s_{2}\mathcal{i}&\mathcal{h}s_{1}s_{3}s_{2}\mathcal{i}&s_{1}s_{3}\\ &\mathcal{Z}&\widehat{s_{2}s_{3}s_{2}}&\widehat{s_{2}s_{3}}&\widehat{s_{2}s_{3}}&\widehat{s_{2}s_{1}}\cup\{s_{2}s_{3}\}&\widehat{s_{2}s_{1}}\cup\{s_{2}s_{3}\}&\\ \hline\cr\tilde{c}_{3},&\mathcal{T}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&\{e\}&\{e\}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&s_{1}\\ &\mathcal{Z}&\widehat{s_{2}s_{3}s_{2}}&\widehat{s_{2}s_{3}s_{2}}&\widehat{s_{2}s_{3}}&\widehat{s_{2}s_{3}}&\widehat{s_{2}s_{3}s_{2}}&\\ \hline\cr\tilde{c}_{4},&\mathcal{T}&\{e\}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&s_{2}s_{3}s_{2}s_{3}\\ &\mathcal{Z}&\{e\}&\widehat{s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{3}}&\\ \hline\cr\tilde{c}_{5},&\mathcal{T}&\{e\}&\{e\}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\{e\}&s_{2}s_{3}s_{2}\\ &\mathcal{Z}&\{e\}&\{e\}&\widehat{s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{3}}&\{e\}&\\ \hline\cr\tilde{c}_{6},&\mathcal{T}&\{e\}&\{e\}&\{e\}&\{e\}&\{e\}&s_{2}\\ &\mathcal{Z}&\widehat{s_{3}}&\widehat{s_{3}}&\widehat{s_{3}}&\widehat{s_{3}}&\widehat{s_{3}}&\\ \hline\cr\tilde{c}_{7},&\mathcal{T}&\{e\}&\{e\}&\{e\}&\{e\}&\{e\}&s_{3}\\ &\mathcal{Z}&\{e\}&\{e\}&\{e\}&\{e\}&\{e\}&\\ \hline\cr\end{array}



Generic parameters in zone BiB_{i} (i=1,2i=1,2).

Table 9. Partition 𝒫LR,\mathcal{P}_{LR,\mathfrak{C}} and values of the 𝐚\mathbf{a}-function

c8={e}0c7={s3}cc6={s1}ac5={s1s3}a+cc4={s2,s1s2,s2s1,s1s2s1,s3s2,s2s3,s3s2s3}bc3={s2s1s2}2bac2={s2s3s2}2bcc1={w2,3}2b+2cc0={w1,2}2a+2b\begin{array}[]{|l|c|}\hline\cr c_{8}=\{e\}&0\\ c_{7}=\{s_{3}\}&c\\ c_{6}=\{s_{1}\}&a\\ c_{5}=\{s_{1}s_{3}\}&a+c\\ c_{4}=\{s_{2},s_{1}s_{2},s_{2}s_{1},s_{1}s_{2}s_{1},s_{3}s_{2},s_{2}s_{3},s_{3}s_{2}s_{3}\}&b\\ c_{3}=\{s_{2}s_{1}s_{2}\}&2b-a\\ c_{2}=\{s_{2}s_{3}s_{2}\}&2b-c\\ c_{1}=\{w_{2,3}\}&2b+2c\\ c_{0}=\{w_{1,2}\}&2a+2b\\ \hline\cr\end{array}

Table 10. Partition 𝒫\mathcal{P}_{\mathfrak{C}}

(r1,r2)B2c0c1c2c3c4c5c6c7c8(r1,r2)B1c0c1c2c3c5c4c6c7c8\begin{array}[]{|c|ccccccccc|}\hline\cr(r_{1},r_{2})\in B_{2}&c_{0}&c_{1}&c_{2}&c_{3}&c_{4}&c_{5}&c_{6}&c_{7}&c_{8}\\ \hline\cr(r_{1},r_{2})\in B_{1}&c_{0}&c_{1}&c_{2}&\lx@intercol c_{3}\leftrightarrow c_{5}\hfil\lx@intercol&c_{4}&c_{6}&c_{7}&c_{8}\\ \hline\cr\end{array}

Table 11. The sets 𝒯\mathcal{T} and 𝒵\mathcal{Z}

B1B2wcc~1,𝒯𝒽s2s3s2s1𝒾𝒽s2s3s2s1𝒾s2s3s2s3𝒵s1s2s3^s1s2s3^c~2,𝒯𝒽s2s3s2s1𝒾𝒽s2s3s2s1𝒾s2s3s2𝒵s1s2s3^s1s2s3^c~3,𝒯{e}{e}s2s1s2𝒵s3^s3^c~4,𝒯{e}𝒽s2s1s3𝒾s2𝒵{e,s1,s3}s1s3^c~5,𝒯𝒽s1s3s2𝒾{e}s1s3𝒵s2s1^{s2s3}{e}c~6,𝒯{e}{e}s1𝒵{e}{e}c~7,𝒯{e}{e}s3𝒵{e}{e}\begin{array}[]{|cc|c|c|c|c|c|}\hline\cr&&B_{1}&B_{2}&w_{c}\\ \hline\cr\tilde{c}_{1},&\mathcal{T}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&s_{2}s_{3}s_{2}s_{3}\\ &\mathcal{Z}&\widehat{s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{3}}&\\ \hline\cr\tilde{c}_{2},&\mathcal{T}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&s_{2}s_{3}s_{2}\\ &\mathcal{Z}&\widehat{s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{3}}&\\ \hline\cr\tilde{c}_{3},&\mathcal{T}&\{e\}&\{e\}&s_{2}s_{1}s_{2}\\ &\mathcal{Z}&\hat{s_{3}}&\hat{s_{3}}&\\ \hline\cr\tilde{c}_{4},&\mathcal{T}&\{e\}&\mathcal{h}s_{2}s_{1}s_{3}\mathcal{i}&s_{2}\\ &\mathcal{Z}&\{e,s_{1},s_{3}\}&\widehat{s_{1}s_{3}}&\\ \hline\cr\tilde{c}_{5},&\mathcal{T}&\mathcal{h}s_{1}s_{3}s_{2}\mathcal{i}&\{e\}&s_{1}s_{3}\\ &\mathcal{Z}&\widehat{s_{2}s_{1}}\cup\{s_{2}s_{3}\}&\{e\}&\\ \hline\cr\tilde{c}_{6},&\mathcal{T}&\{e\}&\{e\}&s_{1}\\ &\mathcal{Z}&\{e\}&\{e\}&\\ \hline\cr\tilde{c}_{7},&\mathcal{T}&\{e\}&\{e\}&s_{3}\\ &\mathcal{Z}&\{e\}&\{e\}&\\ \hline\cr\end{array}


Generic parameters in zone CiC_{i} (i=1,2,3i=1,2,3).

Table 12. Partition 𝒫LR,\mathcal{P}_{LR,\mathfrak{C}} and values of the 𝐚\mathbf{a}-function

c8={e}0c7={s2}bc6={s3,s2s3,s3s2,s2s3s2}cc5={s3s2s3}2cbc4={s2s3s2s3}2b+2cc3={s1,s2s1,s1s2,s2s1s2}ac2={s1s3}a+cc1={s1s2s1}2abc0={w1,2}2a+2b\begin{array}[]{|l|c|}\hline\cr c_{8}=\{e\}&0\\ c_{7}=\{s_{2}\}&b\\ c_{6}=\{s_{3},s_{2}s_{3},s_{3}s_{2},s_{2}s_{3}s_{2}\}&c\\ c_{5}=\{s_{3}s_{2}s_{3}\}&2c-b\\ c_{4}=\{s_{2}s_{3}s_{2}s_{3}\}&2b+2c\\ c_{3}=\{s_{1},s_{2}s_{1},s_{1}s_{2},s_{2}s_{1}s_{2}\}&a\\ c_{2}=\{s_{1}s_{3}\}&a+c\\ c_{1}=\{s_{1}s_{2}s_{1}\}&2a-b\\ c_{0}=\{w_{1,2}\}&2a+2b\\ \hline\cr\end{array}

Table 13. Partition 𝒫\mathcal{P}_{\mathfrak{C}}

(r1,r2)C1c0c4c2c1c3c5c6c7c8(r1,r2)C2c0c1c4c2c3c5c6c7c8(r1,r2)C3c0c1c2c3c4c5c6c7c8\begin{array}[]{|c|ccccccccc|}\hline\cr(r_{1},r_{2})\in C_{1}&c_{0}&c_{4}&c_{2}&c_{1}&c_{3}&c_{5}&c_{6}&c_{7}&c_{8}\\ \hline\cr(r_{1},r_{2})\in C_{2}&c_{0}&\lx@intercol\hfil c_{1}\leftrightarrow c_{4}\lx@intercol&c_{2}&c_{3}&c_{5}&c_{6}&c_{7}&c_{8}\\ \hline\cr(r_{1},r_{2})\in C_{3}&c_{0}&c_{1}&c_{2}&\lx@intercol\hfil c_{3}\leftrightarrow c_{4}\lx@intercol&c_{5}&c_{6}&c_{7}&c_{8}\\ \hline\cr\end{array}

Table 14. The sets 𝒯\mathcal{T} and 𝒵\mathcal{Z}

C1C2C3wcc~1,𝒯{e}𝒽s1s2s3𝒾𝒽s1s2s3𝒾s1s2s1𝒵{e}s3s2s3^s3s2s3^c~2,𝒯𝒽s1s3s2𝒾{e}𝒽s1s2s3s2𝒾s1s3𝒵s2s1^{s2s3}s2s3^s2s3s2^c~3,𝒯𝒽s1s2s3s2𝒾𝒽s1s2s3s2𝒾𝒽s1s2s3s2𝒾s1𝒵s2s3s2^s2s3s2^s2s3s2^c~4,𝒯𝒽s2s3s2s1𝒾𝒽s2s3s2s1𝒾{e}s2s3s2s3𝒵s1s2s3^s1s2s3^{e}c~5,𝒯{e}{e}{e}s3s2s3𝒵{e}{e}{e}c~6,𝒯{e}{e}{e}s3𝒵s2^s2^s2^c~7,𝒯{e}{e}{e}s2𝒵{e}{e}{e}\begin{array}[]{|cc|c|c|c|c|c|}\hline\cr&&C_{1}&C_{2}&C_{3}&w_{c}\\ \hline\cr\tilde{c}_{1},&\mathcal{T}&\{e\}&\mathcal{h}s_{1}s_{2}s_{3}\mathcal{i}&\mathcal{h}s_{1}s_{2}s_{3}\mathcal{i}&s_{1}s_{2}s_{1}\\ &\mathcal{Z}&\{e\}&\widehat{s_{3}s_{2}s_{3}}&\widehat{s_{3}s_{2}s_{3}}&\\ \hline\cr\tilde{c}_{2},&\mathcal{T}&\mathcal{h}s_{1}s_{3}s_{2}\mathcal{i}&\{e\}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&s_{1}s_{3}\\ &\mathcal{Z}&\widehat{s_{2}s_{1}}\cup\{s_{2}s_{3}\}&\widehat{s_{2}s_{3}}&\widehat{s_{2}s_{3}s_{2}}&\\ \hline\cr\tilde{c}_{3},&\mathcal{T}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&\mathcal{h}s_{1}s_{2}s_{3}s_{2}\mathcal{i}&s_{1}\\ &\mathcal{Z}&\widehat{s_{2}s_{3}s_{2}}&\widehat{s_{2}s_{3}s_{2}}&\widehat{s_{2}s_{3}s_{2}}&\\ \hline\cr\tilde{c}_{4},&\mathcal{T}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\mathcal{h}s_{2}s_{3}s_{2}s_{1}\mathcal{i}&\{e\}&s_{2}s_{3}s_{2}s_{3}\\ &\mathcal{Z}&\widehat{s_{1}s_{2}s_{3}}&\widehat{s_{1}s_{2}s_{3}}&\{e\}&\\ \hline\cr\tilde{c}_{5},&\mathcal{T}&\{e\}&\{e\}&\{e\}&s_{3}s_{2}s_{3}\\ &\mathcal{Z}&\{e\}&\{e\}&\{e\}&\\ \hline\cr\tilde{c}_{6},&\mathcal{T}&\{e\}&\{e\}&\{e\}&s_{3}\\ &\mathcal{Z}&\hat{s_{2}}&\hat{s_{2}}&\hat{s_{2}}&\\ \hline\cr\tilde{c}_{7},&\mathcal{T}&\{e\}&\{e\}&\{e\}&s_{2}\\ &\mathcal{Z}&\{e\}&\{e\}&\{e\}&\\ \hline\cr\end{array}

References

  • [1] C. Bonnafé. Semicontinuity properties of Kazhdan-Lusztig cells. New-Zealand Journal of Mathematics 39, 171-192, 2009.
  • [2] N. Bourbaki. Groupes et algèbres de Lie, Chap 4–6. Hermann, Paris, 1968; Masson, Paris, 1981.
  • [3] M. Geck. On the induction of Kazhdan-Lusztig cells. Bull. London Math. Soc. 35, 608–614, 2003.
  • [4] M. Geck. Hecke algebras of finite type are cellular. Invent. Math. 169, 501–517, 2007.
  • [5] J. J. Graham and G. I. Lehrer. Cellular algebras. Invent. Math., 123, 1–34, 1996.
  • [6] J. Guilhot. Some computations about Kazhdan-Lusztig cells in affine Weyl groups of rank 2. available at http://arxiv.org/abs/0810.5165.
  • [7] J. Guilhot. Generalized induction of Kazhdan-Lusztig cells. Ann. Inst. Fourier, 59 p. 1385-1412, 2009.
  • [8] J. Guilhot. Kazhdan-Lusztig cells in affine Weyl groups of rank 2. Int Math Res Notices Vol. 2010 3422-3462, 2010.
  • [9] S. Koenig and C. Xi. Affine cellular algebras. preprint available at http://math.bnu.edu.cn/ ccxi/Papers/Articles/affcell.pdf.
  • [10] G. Lusztig. Hecke algebras and Jantzen’s generic decomposition patterns. Adv. in Math. 𝟑𝟕\mathbf{37}, 121–164, 1980.
  • [11] G. Lusztig. Hecke algebras with unequal parameters. CRM Monograph Series 𝟏𝟖\mathbf{18}, Amer. Math. Soc., Providence, RI, 2003.
  • [12] E. Opdam and M.  Solleveld. Homological algebra for affine Hecke algebras. Adv. Math. 220, no. 5, 1549–1601, 2009.