Hecke algebras of double cosets
For a compact open subgroup $J$ of $\GF$, the functions on $J\backslash\GF/J$ form an algebra under convolution. This page defines it, proves the three general facts the Concept needs (structure constants are counts, the integral is a character, the index is the integral), and shows the finite Hecke algebra inside the Iwahori one.
| object | type | defined in |
|---|---|---|
| $J$ | a compact open subgroup of $\GF$ (on this site $J=I$ or $J=K$) | §1 |
| $dg$, $\vol$ | the Haar measure on $\GF$ with $\vol(J)=1$ | §1 |
| $\Cc(J\backslash\GF/J)$ | a $\C$-vector space with basis the indicator functions of double cosets | §1 |
| $\ast:\cH_J\times\cH_J\to\cH_J$ | convolution | §2 |
| $\ind:\cH_J\to\C$ | the integral, an algebra homomorphism | §3 |
| $\Cc(J\backslash Y)$ | a left $\cH_J$-module, for a $\GF$-set $Y$ | §4 |
| $\Hzero\subset\cH$ | the finite Hecke algebra inside the Iwahori one | §5 |
The Hecke algebra of a compact open subgroup Definition
(Hecke algebra) [HKP10, §1.2], [IM65, §3.1]
Let $J\subset\GF$ be a compact open subgroup and $dg$ the Haar measure on $\GF$ with $\vol(J)=1$. Put
$$\cH_J=\Cc(J\backslash\GF/J)=\{f:\GF\to\C\ \text{ with compact support, }\ f(j_1gj_2)=f(g)\ \text{ for }j_1,j_2\in J\}.$$It has the basis $\one_{JxJ}$, one for each double coset; on this site $\cH=\cH_I$ and $\HK=\cH_K$.
Each double coset $JxJ$ is compact and open, so it is a finite union of left cosets $yJ$; the number of them is finite because $JxJ$ is compact and the $yJ$ are open. A function with compact support that is $J$-invariant on both sides is therefore a finite linear combination of the $\one_{JxJ}$, which are linearly independent since the double cosets are disjoint.
Convolution Proved here
(convolution) [HKP10, §1.2, footnote 1]
For $f\in\cH_J$ and a left $J$-invariant function $\varphi$ on a $\GF$-set (for instance $\varphi\in\cH_J$),
($\cH_J$ is an algebra; structure constants are counts) Proved here
a number that depends only on the double coset of $z$, and is zero unless $JzJ\subseteq JxJ\cdot JyJ$.
Proof
- The summand depends only on $yJ$: $f(yj)=f(y)$ and $\varphi(j^{-1}y^{-1}x)=\varphi(y^{-1}x)$. Only the finitely many cosets $yJ\subseteq\supp(f)$ contribute. For $j\in J$, $(f\ast\varphi)(jx)=\sum_y f(y)\varphi(y^{-1}jx)=\sum_{y'}f(jy')\varphi(y'^{-1}x)$ with $y'=j^{-1}y$, and $f(jy')=f(y')$. If $(f\ast\varphi)(x)\neq0$ then $x=y\cdot(y^{-1}x)$ with $y\in\supp f$ and $y^{-1}x\in\supp\varphi$.
- Associativity is Fubini for the sum over $\GF/J\times\GF/J$; $(\one_J\ast\varphi)(x)=\sum_{y\in J/J}\varphi(y^{-1}x)=\varphi(x)$, and likewise on the right.
- $(\one_{JxJ}\ast\one_{JyJ})(z)=\sum_{u\in\GF/J}\one_{JxJ}(u)\one_{JyJ}(u^{-1}z)$ is the count $c^{z}_{x,y}$. It is right $J$-invariant in $z$ by (i) applied on the other side (the same computation with $x\mapsto xj$), so it is constant on $JzJ$; it vanishes unless $z\in JxJ\cdot JyJ$.
This is the multiplication law of [IM65, p. 276], where $c^{z}_{x,y}$ is written $m^{\mu}_{\sigma,\tau}=|B\backslash B\omega(\sigma)^{-1}B\omega(\mu)\cap B\omega(\tau)B|$.
The index of a double coset and the integral Proved here
(index) [IM65, §3.1]
$$\ind(x)=|JxJ/J|=[J:J\cap x^{-1}Jx]=\int_{\GF}\one_{JxJ}\,dg,\qquad \ind\Big(\sum_x\lambda_x\one_{JxJ}\Big)=\sum_x\lambda_x\ind(x).$$(the integral is a character) [IM65, p. 276] Proved here
so $\ind:\cH_J\to\C$ is an algebra homomorphism. In particular $\ind(x)\,\ind(y)=\sum_z c^{z}_{x,y}\,\ind(z)$.
Proof
- $\int(f\ast g)(x)\,dx=\int\!\!\int f(y)g(y^{-1}x)\,dy\,dx$. For fixed $y$, substitute $x=yx'$: the Haar measure is left invariant, so the inner integral is $\int g(x')dx'=\ind(g)$.
- Hence $\int f\ast g=\ind(f)\ind(g)$. The three expressions for $\ind(x)$ agree because $JxJ=\bigsqcup_{u}uJ$ over $u\in JxJ/J$, each $uJ$ has volume $1$, and $u\mapsto u$ identifies $JxJ/J$ with $J/(J\cap xJx^{-1})$ via $j\mapsto jxJ$.
Only left invariance of $dg$ is used. ($\GF$ is unimodular, but this is not needed.)
This character is the tool that turns a support statement into an equation: if $\one_{JxJ}\ast\one_{JyJ}=c\,\one_{JzJ}$ for a single $z$, then $c=\ind(x)\ind(y)/\ind(z)$. The Concept uses it in exactly this way (the Concept §4).
Modules of invariant functions Definition
The same formula with $\varphi$ a left $J$-invariant compactly supported function on a $\GF$-set $Y$ with open stabilizers makes $\Cc(J\backslash Y)$ a left $\cH_J$-module: $f\ast(g\ast\varphi)=(f\ast g)\ast\varphi$ by the same Fubini argument. Two cases matter on these pages and in the proof workspace:
- $Y=\GF/J'$ for a second compact open subgroup $J'$: then $\Cc(J\backslash\GF/J')$ is an $(\cH_J,\cH_{J'})$-bimodule. For $J=I$, $J'=K$ this is the module of Iwahori–spherical translates.
- $Y=X(F)$ for a $G$-variety $X$: $\Cc(J\backslash X(F))$ is the module whose generation the proof workspace studies [Draft].
The finite Hecke algebra inside the Iwahori one Proved (cited)
($\Hzero\subset\cH$) [HKP10, §1.7] Proved here
The functions supported on $K$ form a subalgebra
$$\Hzero=\Cc(I\backslash K/I)\ \subset\ \cH,\qquad \Hzero\simeq\C\big[B(\Fq)\backslash G(\Fq)/B(\Fq)\big],$$with basis $T_w=\one_{IwI}$, $w\in W$, and $\one_K=\sum_{w\in W}T_w$.
Proof
$K$ is a group, so $\supp(f\ast g)\subseteq K$ when both supports lie in $K$ ((i)). Pull back the Bruhat decomposition $G(\Fq)=\bigsqcup_{w\in W}B(\Fq)wB(\Fq)$ along $\ev$: $K=\bigsqcup_{w\in W}IwI$, which gives the basis and the formula for $\one_K$. Functions on $I\backslash K/I$ are functions on $B(\Fq)\backslash G(\Fq)/B(\Fq)$ because $\ker\ev\subseteq I$, and the convolutions agree since $\vol(I)=1$ corresponds to counting cosets of $B(\Fq)$.
This is Iwahori's 1964 algebra (History) sitting inside the affine one. The Concept shows that its relations are the same quadratic relations, now for all $s\in\Saff$ rather than $s\in S$.
How this page meets the Concept Context
With $J=I$, the basis of $\cH$ is $\{T_w\}_{w\in\Wt}$ by the Iwahori–Bruhat decomposition (Groups §6). The Concept computes the structure constants $c^{z}_{s,w}$ for $s\in\Saff$: (ii) says which $z$ can occur, and fixes the coefficients once the index $\ind(w)=q^{\len(w)}$ is known.