Groups and the affine Weyl group
The local field, the group $\GF$, its two compact open subgroups $K\supset I$, and the group $\Wt$ that indexes the double cosets of $I$. Each object is defined, then shown for the running example $\SL_2$.
| object | type | defined in |
|---|---|---|
| $F$, $\cO$, $t$, $q$ | a local field, its integers, a uniformizer, the size of the residue field | §1 |
| $G\supset B\supset T$ | a split reductive group, a Borel subgroup, a maximal torus, all over $\cO$ | §1 |
| $\ev:K\to G(\Fq)$ | reduction modulo $t$ on $K=G(\cO)$ | §1 |
| $I\subset K$ | the Iwahori subgroup, a compact open subgroup of $\GF$ | §2 |
| $\Wt$, $\Waff$, $\Om$ | groups: $\Xs\rtimes W$, its Coxeter subgroup, the stabilizer of an alcove | §3, §5 |
| $\len:\Wt\to\N$ | the length function | §5 |
| $\GF=\bigsqcup_{w\in\Wt}IwI$ | the Iwahori–Bruhat decomposition | §6 |
The local field and the groups Definition
(the setting)
Let $q$ be a prime power and
$$F=\Fq((t)),\qquad\cO=\Fq[[t]],\qquad\cO/t\cO=\Fq .$$Let $G$ be a split connected reductive group over $\cO$ with a split maximal torus $T$ and a Borel subgroup $B=TU$ containing it, $U$ its unipotent radical. Write $W=N_G(T)/T$ for the finite Weyl group and $\Xs=\Hom(\mathbb G_m,T)$ for the cocharacter lattice. Put
$$K=G(\cO)\subset\GF,\qquad\ev:K\longrightarrow G(\Fq)\ \text{ the reduction modulo }t .$$$F$ is a local field: complete for the $t$-adic absolute value, with finite residue field. Only two properties of it are used on these pages: $\cO$ is compact and open in $F$, and $\cO/t^n\cO$ is finite with $q^n$ elements. So $\GF$ is a locally compact totally disconnected group, and $K$ is a compact open subgroup. The theory is the same for the $p$-adic fields of the sources [HKP10, p. 1].
The Iwahori subgroup Definition
(Iwahori subgroup) [HKP10, p. 1], [IM65, §1.1]
$$I=\ev^{-1}\big(B(\Fq)\big)=\{g\in G(\cO):\ \ev(g)\in B(\Fq)\}\ \subset\ K .$$$I$ is open in $K$ because it contains the kernel of $\ev$, and it has finite index: $K/I\simeq G(\Fq)/B(\Fq)$, the flag variety over the residue field. Iwahori and Matsumoto write $B$ for it and define it by generators [IM65, §1.1]; the two definitions agree by their Theorem 2.5, which is the Iwahori factorization $I=U^-(t\cO)\,T(\cO)\,U(\cO)$ in the notation of SL₂ I §4.
(index of $I$ in $K$) Proved here
$$[K:I]=|G(\Fq)/B(\Fq)|=\sum_{w\in W}q^{\len(w)} .$$Proof
$\ev$ is surjective because $G$ is smooth over $\cO$ (Hensel's lemma), so $K/I\to G(\Fq)/B(\Fq)$ is a bijection. The Bruhat decomposition $G(\Fq)=\bigsqcup_{w\in W}B(\Fq)wB(\Fq)$ and the count $|B(\Fq)wB(\Fq)/B(\Fq)|=q^{\len(w)}$ (the big cell of $wB/B$ is an affine space of dimension $\len(w)$) give the sum. The same number appears as $W(q)$ in [HKP10, proof of Thm 5.6.1, p. 15].
The extended affine Weyl group Definition
(extended affine Weyl group) [HKP10, §1.1]
$$\Wt=N_G(T)(F)\,/\,T(\cO)\ \simeq\ \Xs\rtimes W,\qquad \mu\longmapsto t^{\mu}:=\mu(t)\in T(F).$$The map $\mu\mapsto t^\mu$ identifies $\Xs$ with $T(F)/T(\cO)$, the translation subgroup; $W=N_G(T)(\cO)/T(\cO)$ is a complement.
Elements of $\Wt$ are not elements of $\GF$, but every $w\in\Wt$ has representatives $\dot w\in N_G(T)(F)$, and any two differ by an element of $T(\cO)\subset I$. So the double coset $I\dot wI$ depends only on $w$; it is written $IwI$.
Alcoves and the affine Weyl group Definition
$\Wt$ acts on the real vector space $V=\Xs\otimes\R$ by affine maps: $W$ linearly and $\mu\in\Xs$ by translation $x\mapsto x+\mu$. For each root $\alpha$ and integer $k$, the affine root hyperplane is
$$H_{\alpha,k}=\{x\in V:\ \langle\alpha,x\rangle=k\},$$and the reflection in it is $s_{\alpha,k}(x)=x-(\langle\alpha,x\rangle-k)\alpha^\vee=t^{k\alpha^\vee}s_\alpha$ [IM65, §1.1].
(alcoves, $\Waff$) [IM65, §1.3–1.4], [HKP10, §7.1]
An alcove is a connected component of $V\smallsetminus\bigcup_{\alpha,k}H_{\alpha,k}$. The fundamental alcove and the affine Weyl group are
$$A_0=\{x\in V:\ -1<\langle\alpha,x\rangle<0\ \text{ for every positive root }\alpha\},\qquad \Waff=\Qv\rtimes W\subset\Wt,$$where $\Qv\subset\Xs$ is the coroot lattice. $\Waff$ is generated by the reflections in the walls of $A_0$: the simple reflections $S$ of $W$ together with $s_0=s_{\tilde\alpha,-1}=t^{-\tilde\alpha^\vee}s_{\tilde\alpha}$ for the highest root $\tilde\alpha$ (one such reflection per simple factor of $G$). Write $\Saff=S\cup\{s_0\}$.
$A_0$ is taken in the negative Weyl chamber, with $0$ in its closure, because $I$ is the inverse image of $B$ and not of the opposite Borel subgroup: with this choice the walls of $A_0$ are the reflections $s$ whose double cosets $IsI$ are the minimal ones outside $I$, as the Concept shows [HKP10, footnote 2, p. 3, and §7.1]. Defining $I$ with the opposite Borel subgroup would replace $A_0$ by $-A_0$.
(simple transitivity) [IM65, Prop 1.2, Cor 1.8, Cor 1.16] Proved (cited)
$\Waff$ is generated by $\Saff$ and acts simply transitively on the set of alcoves; it is a Coxeter group with the relations $s^2=1$ and the braid relations $(st)^{m_{st}}=1$ determined by the angles between the walls of $A_0$.
Proof
Proof idea
Transitivity: an alcove is moved to $A_0$ by successively reflecting in a wall of $A_0$ that separates it from $A_0$, which strictly decreases the number of hyperplanes between them [IM65, proof of Prop 1.1]. Freeness: an element fixing $A_0$ separates it from itself by no hyperplane, and a non-identity reduced word always crosses at least one [IM65, Lemma 1.7, Cor 1.8]. The presentation is [IM65, Cor 1.16].
Length, reduced words, and the length-zero subgroup $\Om$ Definition
(length, $\Om$) [IM65, §1.4, §1.7]
$$\len(w)=\#\{H_{\alpha,k}:\ H_{\alpha,k}\ \text{separates}\ A_0\ \text{from}\ wA_0\},\qquad \Om=\{w\in\Wt:\ wA_0=A_0\}=\{w\in\Wt:\len(w)=0\}.$$A reduced expression of $w\in\Waff$ is a word $w=s_{i_1}\cdots s_{i_r}$ in $\Saff$ of minimal length $r$.
(length is word length; $\Wt=\Waff\rtimes\Om$) [IM65, Prop 1.10, §1.7] Proved (cited)
Proof
Proof idea
(i) Each letter of a word crosses one wall, so $\len(w)\le$ word length; conversely a word of length $\len(w)$ is produced by the reflection procedure of [IM65, Cor 1.6, Prop 1.10]. (ii) The wall $H_s$ of $A_0$ either separates $A_0$ from $wA_0$ or not, and $s$ changes exactly that one count [IM65, Lemma 1.5]. (iii) Simple transitivity gives $\Wt=\Om\cdot\Waff$ with $\Om\cap\Waff=1$; the quotient $\Wt/\Waff=\Xs/\Qv$ [IM65, §1.7].
$\Om$ is the fundamental group of $G$ in the sense of root data: trivial when $G$ is simply connected, $\Z/(n)$ for $\PGL_n$, $\Z$ for $\GL_n$. The extended group $\Wt$ is not a Coxeter group when $\Om\neq1$, but it is one up to the finite group $\Om$, which is why the Hecke algebra is a twisted tensor product (the Concept).
The Iwahori–Bruhat decomposition Proved (cited)
(Iwahori–Bruhat decomposition) [IM65, Thm 2.16] Proved (cited)
Moreover, for $s\in\Saff$ and $w\in\Wt$ [IM65, Prop 2.8]:
Proof
Proof idea, and where it is proved in full
Iwahori and Matsumoto prove it for Chevalley groups. Every $g\in\GF$ lies in some $K\,t^{\mu}K$ (Cartan decomposition), and $K=\bigsqcup_{w\in W}IwI$ by the Bruhat decomposition of $G(\Fq)$ pulled back along $\ev$; the products of double cosets are controlled by the rank-one computation in $\SL_2$ applied to each simple affine root, which is (a) and (b) [IM65, Prop 2.6, Prop 2.8]. Disjointness is an induction on length using (a) and (b) [IM65, Prop 2.13]. For $\SL_2$ the whole statement is checked by hand on SL₂ I §2–3. For a general split reductive group it is part of Bruhat–Tits theory, and [HKP10, §1.2] takes it as known.
How these objects meet the next page Context
The decomposition says that the functions on $\GF$ invariant under $I$ on both sides have a basis of indicator functions $T_w=\one_{IwI}$, one per element of $\Wt$. The next page makes these functions into an algebra by convolution, and the Concept computes the products $T_sT_w$ from (a)–(c) and the count $|IwI/I|=q^{\len(w)}$.