Definitions
The action correspondence is \(m:LG\times^I LX\to LX\), \([g,y]\mapsto gy\), and \(\mathcal G*_IM=m_!(\mathcal G\widetilde\boxtimes M)\). A trace is the alternating Frobenius trace on stalk cohomology. Write \(\mathbb F_q\) for the residue field and \(F=\mathbb F_q(\!(t)\!)\).
Hypotheses
Use (Lev) and (Dict). The bounded kernel descends to a finite-type model and the Schubert support is proper. The relevant Iwahori congruence quotients are connected, so Lang's theorem identifies rational flag points with \(G(F)/I\).
Lemma IIb · Trace of convolution. Let \(\mathcal G\in\mathcal H_{c,I}\) have support in \(\mathrm{Fl}_{\le w}\), and let \(M\in\mathcal C_I\) be a Weil object. Use (Dict)(d), the induced Weil kernel and Haar normalization \(\operatorname{vol}I=1\).
$$\operatorname{tr}(\mathcal G\ast_IM)=\operatorname{tr}\mathcal G\ast\operatorname{tr}M,\qquad(\operatorname{tr}\mathcal G\ast\operatorname{tr}M)(x)=\sum_{gI\in G(F)/I}\operatorname{tr}(\mathcal G)(g)\,\operatorname{tr}(M)(g^{-1}x),\qquad\operatorname{tr}\mathrm{IC}_0=\varphi_0 .$$Steps 1–3 · Finite correspondence · Steps 4–6 · Frobenius traces
Finite correspondence
Rewrite the action map
Shearing identifies the correspondence with a projection.
$$[g,y]\longmapsto(gI,gy),\qquad LG\times^ILX\simeq\mathrm{Fl}\times LX,\qquad m=\mathrm{pr}_2.$$Proof
- The relation \((g,y)\sim(gi,i^{-1}y)\) leaves both \(gI\) and \(gy\) unchanged.
- The inverse sends \((gI,x)\) to \([g,g^{-1}x]\), independently of the representative.
- Both maps are defined over the residue field and commute with Frobenius.
Sources
Identify the kernel stalk
The descended twisted external product has stalk
$$K_{(gI,x)}\simeq\mathcal G_g\otimes M_{g^{-1}x}.$$Proof
- Pull back to \(LG\times LX\), where the twisted product becomes the ordinary external product.
- Apply the inverse shearing map. Equivariance identifies the stalks when \(g\) is replaced by \(gi\).
- Descent preserves this tensor description and its Frobenius action.
Sources
Choose a finite model
Choose \(N\) supporting \(M\); (Dict)(d) supplies \(N'\) and \(M''\).
$$\operatorname{supp}K\subseteq\mathrm{Fl}_{\le w}\times Y_{N'},\qquad K=\operatorname{pullback}(K_{N',M''}).$$Proof
- The support bound places every output in \(Y_{N'}\).
- The factorization requirement in (Dict)(d) makes the kernel depend on finitely many output coefficients.
- The descended projection is proper because \(\mathrm{Fl}_{\le w}\) is projective. Proper base change now computes the stalk at \(x\) on this finite-type model.
Sources
Frobenius traces
Apply the trace formula
$$\operatorname{tr}(\mathcal G*_IM)(x)=\sum_{gI\in\mathrm{Fl}_{\le w}(\mathbb F_q)}\operatorname{tr}(\mathcal G_g)\operatorname{tr}(M_{g^{-1}x}).$$Proof
- Proper base change identifies the output stalk with the cohomology of the fibre.
- Grothendieck–Lefschetz replaces its alternating Frobenius trace by the sum of stalk traces over rational fibre points.
- The alternating trace of a tensor product is the product of alternating traces. The support has finitely many rational points.
Sources
Identify rational cosets
$$\mathrm{Fl}(\mathbb F_q)=G(F)/I,\qquad\operatorname{tr}(\mathcal G*_IM)=\operatorname{tr}\mathcal G*\operatorname{tr}M.$$Proof
- The obstruction to representing a rational flag by a rational loop lies in \(H^1(\mathbb F_q,I)\).
- Lang's theorem kills this obstruction on the connected finite congruence quotients; compatible lifts through the pro-unipotent kernels give the same conclusion for \(I\).
- Each right coset has measure one under \(\operatorname{vol}I=1\). The sum in Step 4 is therefore the usual convolution integral.
Sources
Check a valuation translate
For \(X=\mathbb A^1\), \(G=\mathrm{GL}_1\), the flag space is discrete.
$$I=\mathcal O^\times,\quad\mathrm{Fl}(\mathbb F_q)=\{t^jI:j\in\mathbb Z\},\quad\mathcal G=\delta_{t^j},\quad M=\overline{\mathbb Q}_{\ell,\mathcal O}.$$Proof
- Only the coset \(t^jI\) contributes.
- The action is the isomorphism \(y\mapsto t^jy\) from \(\mathcal O\) onto \(t^j\mathcal O\).
- With the unshifted constant Weil structures,
For \(j=1\), the trace is one precisely when the constant coefficient of \(x\in\mathcal O\) vanishes. This is the trace calculation used in III.
Sources