The length-zero subgroup

What does the result in Haines–Kottwitz–Prasad say, and why does it give translation?

1 · Reflections and alcove symmetries

· The extended group and Ω Definition

Fix a non-Archimedean local field \(\Loc\), its valuation ring \(\Ring\), and a uniformizer \(\unif\). For a split connected reductive group \(\Grp\) with split maximal torus \(T\), let \(W_0\) be its finite Weyl group and \(Q^\vee\) its coroot lattice. Choose a base alcove \(\alc\) in the apartment, and write

$$\Wext=X_*(T)\rtimes W_0,\qquad \Waff=Q^\vee\rtimes W_0.$$ $$\Om=\operatorname{Stab}_{\Wext}(\alc)=\{w\in\Wext:\len(w)=0\}.$$

Length counts the affine walls separating the base alcove from its image; a central direction contributes no walls.

· The group-algebra part of the Hecke algebra Proved (cited)

With Haar volume of \(\Iw\) equal to one, set

$$\Hecke=C_c(\Iw\backslash\Grp(\Loc)/\Iw),\qquad T_w=\mathbf1_{\Iw w\Iw}.$$ $$\Wext=\Waff\rtimes\Om,\qquad T_\omega T_\eta=T_{\omega\eta}\quad(\omega,\eta\in\Om).$$ $$\mathbb C[\Om]\hookrightarrow\Hecke,\qquad [\omega]\longmapsto T_\omega.$$[HKP, §7.1, p. 19][HKP, §1.2, p. 2]
Proof
  1. Choose a representative of \(\omega\in\Om\) normalizing \(\Iw\); this is the alcove stabilizer description for the split group: $$\Iw\omega\Iw=\omega\Iw.$$
  2. There is only one right coset, and it has volume one: $$T_\omega*T_\eta=\mathbf1_{\omega\eta\Iw}.$$
  3. Different double cosets are disjoint, so their indicators are independent: $$\sum_\omega c_\omega T_\omega=0\ \Longrightarrow\ c_\omega=0\quad\text{for every }\omega.$$

Writing \(\HeckeAff\) for the subalgebra indexed by \(\Waff\), HKP also gives the crossed-product structure:

$$\Hecke\cong\HeckeAff\rtimes\mathbb C[\Om].$$

The twist is conjugation: an alcove symmetry permutes the simple reflection operators.

2 · Why Ω is infinite for GLₙ

· The determinant index Proved here

In the model of the lattice chain, define \(\degdet:\Wext\to\mathbb Z\) by determinant valuation:

$$\degdet(\unif^\lambda w)=\sum_{i=1}^{\nDim}\lambda_i.$$ $$\ker(\degdet)=\Waff,\qquad \degdet(\shift)=1,\qquad \Om=\langle\shift\rangle\cong\mathbb Z.$$ $$\mathbb C[\Om]\cong\mathbb C[z,z^{-1}],\qquad z=T_{\shift}.$$
Proof
  1. The coroot lattice of GLₙ consists of integer vectors of total sum zero: $$Q^\vee=\{\lambda\in\mathbb Z^{\nDim}:\sum_i\lambda_i=0\}.$$
  2. The model proves that \(\shift\) preserves the alcove’s lattice chain, hence has length zero. For every \(w\in\Wext\), removing its determinant degree gives $$w\shift^{-\degdet(w)}\in\Waff.$$
  3. The affine reflection group acts simply transitively on alcoves; an element in it fixing the base alcove is the identity. Therefore $$\Om\cap\Waff=\{1\},\qquad \omega=\shift^{\degdet(\omega)}\quad(\omega\in\Om).$$

Although the affine Dynkin diagram has only \(\nDim\) nodes, \(\shift\) has infinite order: its \(\nDim\)-th power is the nontrivial central translation \(\unif1_{\nDim}\). For \(\nDim=1\), there are no affine walls and the whole extended group is \(\mathbb Z\).

3 · The same operator on any G-space

· Convolution without averaging Proved here

Let \(X(\Loc)\) be a locally compact left \(\Grp(\Loc)\)-space, and define the left Hecke action on \(\Module=C_c^\infty(X(\Loc))^{\Iw}\) by

$$h*f(x)=\int_{\Grp(\Loc)}h(g)f(g^{-1}x)\,dg.$$

For every \(\omega\in\Om\) represented in the normalizer,

$$\boxed{(T_\omega*f)(x)=f(\omega^{-1}x).}$$
Proof
  1. Use the single coset and left invariance of \(f\): $$\int_{\omega\Iw}f(g^{-1}x)\,dg=\int_{\Iw}f(i^{-1}\omega^{-1}x)\,di.$$
  2. The integrand is independent of \(i\), and the volume is one: $$\int_{\Iw}f(i^{-1}\omega^{-1}x)\,di=f(\omega^{-1}x).$$
[HKP, Lemma 7.2.1(iii), p. 19]

HKP uses a right action on a different module. Its inverse in Lemma 7.2.1(iii) reflects that convention; the integral above fixes ours.

For this geometric GLₙ diagram, take \(k=\overline{\mathbb F}_q\) and define the loop functor by \(LX(R)=R((t))^n\) for each k-algebra R. The diagram uses a representative \(\shift^{\idx}\), the quotient maps \(p(g,v)=(gI,v)\), \(q(g,v)=[g,v]\), and action map \(m([g,v])=gv\); the vertical map is \(\phi([\shift^{\idx}i,v])=iv\). The introduction gives the sheaf formula and TikZ source.

Convolution through the contracted product is identified with translation by tau to the a.
Figure 1. For the sheaf action, the contracted product over a length-zero cell identifies the action map with translation.