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arXiv:2607.10073v1 [math.RT] 11 Jul 2026

Base Change Fundamental Lemma FOR CENTRAL ELEMENTS IN DEPTH-ZERO HECKE ALGEBRAS OVER LOCAL FUNCTION FIELDS

Weimin Jiang Address: University of Maryland, College Park
Abstract.

Let GG be an unramified group over a local function field of characteristic p>0p>0. This article introduces an abstract norm map between the twisted conjugacy classes and conjugacy classes of GG in the positive characteristics setting, applies the process of stabilization of (twisted) trace formula and proves the corresponding base change fundamental lemma for regular semisimple elements.

1. Introduction

1.1. Main Results

Let FF denote a local function field of characteristic p>0p>0, and let FrFF_{r}\supset F denote the unique degree rr unramified extension of FF contained in a fixed separable closure FsF^{s} of FF, and let θ\theta denote a generator of Gal(Fr/F)\mathrm{Gal}(F_{r}/F). Let GG denote an unramified connected reductive group over FF. The automorphism θ\theta determines an FF-automorphism of G(Fr)G(F_{r}), which is still denoted by θ\theta. For simplicity, we will assume that Gder=GscG_{\text{der}}=G_{\text{sc}} in the remainder of the introduction.

From the concrete norm map

N:G(Fr)G(Fr)ggθ(g)θr1(g),\begin{split}N:G(F_{r})&\to G(F_{r})\\ g&\mapsto g\theta(g)\dots\theta^{r-1}(g),\end{split}

Kottwitz [30] was able to define an abstract norm map 𝒩\mathcal{N} from the set of stable θ\theta-conjugacy classes in G(Fr)G(F_{r}) to the set of stable conjugacy classes in G(F)G(F) for perfect fields FF. We will say that γG(F)\gamma\in G(F) is a norm if γ\gamma is stably conjugate to NδN\delta for some δG(Fr)\delta\in G(F_{r}), which means that there exist gG(Fs)g\in G(F^{s}) such that g1(Nδ)g=γg^{-1}(N\delta)g=\gamma.

Fix a semisimple element γG(F)\gamma\in G(F) and we let GγGG_{\gamma}\subset G denote its centralizer in GG. For fCc(G(F))f\in C^{\infty}_{c}(G(F)), the algebra of locally constant and compactly supported \mathbb{C}-valued functions on G(F)G(F), we can define the orbital integral

OγG(F)(f)=Gγ(F)\G(F)f(g1γg)𝑑g/𝑑tO^{G(F)}_{\gamma}(f)=\int_{G_{\gamma}(F)\backslash G(F)}f(g^{-1}\gamma g)\,dg/dt

depending on the choice of Haar measures dgdg and dtdt on G(F)G(F) and Gγ(F)G_{\gamma}(F) respectively. We also consider the stable orbital integral

SOγG(F)(f)=γe(Gγ)OγG(F)(f),SO^{G(F)}_{\gamma}(f)=\sum_{\gamma^{\prime}}e(G_{\gamma^{\prime}})O^{G(F)}_{\gamma^{\prime}}(f),

where γ\gamma^{\prime} sums over the conjugacy classes in G(F)G(F) within the stable conjugacy class of γ\gamma, and e(Gγ){±1}e(G_{\gamma^{\prime}})\in\{\pm 1\} is the sign attached by Kottwitz [31] to connected reductive groups. Notice that our assumption that Gder=GscG_{\mathrm{der}}=G_{\mathrm{sc}} implies that the centralizers GγG_{\gamma^{\prime}} are connected. If γ\gamma and γ\gamma^{\prime} are stably conjugate, their centralizers are inner forms of each form, therefore we may require the Haar measures are compatible with each other in the definition of the orbital integrals TOγG(F)(f)TO^{G(F)}_{\gamma^{\prime}}(f) in the sense of [36] p. 631. Similarly, for an element δG(Fr)\delta\in G(F_{r}) such that NδN\delta is semisimple, we define its twisted centralizer to be the connected reductive group GδθG_{\delta\theta} such that

Gδθ(F)={gG(Fr):g1δθ(g)=δ}.G_{\delta\theta}(F)=\{g\in G(F_{r}):g^{-1}\delta\theta(g)=\delta\}.

Then for ϕCc(G(Fr))\phi\in C^{\infty}_{c}(G(F_{r})), similarly we can define the twisted orbital integral

TOδθG(Fr)(ϕ)=Gδθ(F)\G(Fr)ϕ(g1δθ(g))𝑑g/𝑑tTO^{G(F_{r})}_{\delta\theta}(\phi)=\int_{G_{\delta\theta}(F)\backslash G(F_{r})}\phi(g^{-1}\delta\theta(g))\,dg/dt

and its stable version

SOδθG(Fr)(ϕ)=δe(Gδθ)TOδθG(Fr)(ϕ),SO^{G(F_{r})}_{\delta\theta}(\phi)=\sum_{\delta^{\prime}}e(G_{\delta^{\prime}\theta})TO^{G(F_{r})}_{\delta^{\prime}\theta}(\phi),

where the sum is over θ\theta-conjugacy classes δ\delta^{\prime} in G(Fr)G(F_{r}) inside the stable θ\theta-conjugacy class of δ\delta, or equivalently (Proposition 2.16), whose norm down to G(F)G(F) is in the same stable conjugacy class as NδN\delta. If γG(F)\gamma\in G(F) is stably conjugate to NδN\delta, then GδθG_{\delta\theta} is an inner form of GγG_{\gamma} (Lemma 2.5). Therefore we may also require the Haar measures on these groups to be compatible.

We say that ϕCc(G(Fr))\phi\in C^{\infty}_{c}(G(F_{r})) and fCc(G(F))f\in C^{\infty}_{c}(G(F)) are associated or have matching orbital integrals (resp., at regular semisimple elements) if for every (resp., regular) semisimple element γG(F)\gamma\in G(F) we have

(1.1.1) SOγG(F)(f)={SOδθG(Fr)(ϕ)ifγ=𝒩δ0ifγ is not a normSO^{G(F)}_{\gamma}(f)=\left\{\begin{array}[]{rcl}SO^{G(F_{r})}_{\delta\theta}(\phi)&\mbox{if}&\gamma=\mathcal{N}\delta\\ 0&\mbox{if}&\gamma\mbox{ is not a norm}\end{array}\right.

The case of spherical Hecke algebras was studied first. Suppose KrG(Fr)K_{r}\subset G(F_{r}) and KG(F)K\subset G(F) are hyperspecial maximal compact subgroups associated to a hyperspecial vertex in the Bruhat-Tits building (G(F))\mathcal{B}(G(F)) of G(F)G(F), and suppose ϕCc(G(Fr))\phi\in C^{\infty}_{c}(G(F_{r})) belongs to the spherical Hecke algebra (G(Fr),Kr)\mathcal{H}(G(F_{r}),K_{r}) of bi-invariant functions under KrK_{r}. In particular, the spherical Hecke algebras are commutative. The Satake isomorphisms gives rise to a natural algebra homomorphism

(1.1.2) br:(G(Fr),Kr)(G(F),K)b_{r}:\mathcal{H}(G(F_{r}),K_{r})\to\mathcal{H}(G(F),K)

which will be called the base change homomorphism. The base change fundamental lemma for spherical functions asserts that ϕ\phi and br(ϕ)b_{r}(\phi) are associated. This was proved in the special cases of GL2\mathrm{GL}_{2} [45] and GLn\mathrm{GL}_{n} [1], which gave rise to global and local applications, and for general unramified reductive groups it was proved by Clozel [10] and Labesse [42].

In [18], an analogous base change fundamental lemma is proved for centers of parahoric Hecke algebras by Haines, which replaced the hyperspecial maximal compact subgroup KrK_{r} (resp., KK) above by a general parahoric subgroup JrJ_{r} (resp., JJ) defined as intersection of the group of elements in G(Fr)G(F_{r}) (resp. G(F)G(F)) that fix a facet in (G(F))\mathcal{B}(G(F)) with the kernel of Kottwitz homomorphism(see section 2 of loc. cit.). In particular, when the facet is a hyperspecial vertex, we have recovered Jr=KrJ_{r}=K_{r}. However, since the resulting parahoric Hecke algebras (G(Fr),Jr)\mathcal{H}(G(F_{r}),J_{r}) and (G(F),J)\mathcal{H}(G(F),J) are in general no longer commutative, the base change homomorphism will be restricted to the center of those Hecke algebras:

br:𝒵(G(Fr),Kr)𝒵(G(F),K)b_{r}:\mathcal{Z}(G(F_{r}),K_{r})\to\mathcal{Z}(G(F),K)
Remark 1.1.

From now on and in this article, when we speak of base change fundamental lemma, we refer to the matching of elements in the centers of linked by the base change homomorphisms.

Later in [19], Haines generalizes this result to so called depth-zero principal series blocks in the Bernstein decomposition. Generalizing his method, Shenghao Li[46] is able to show the base change fundamental lemma for Bernstein centers of principal series blocks (not just depth-zero ones).

All the results [10, 42, 18, 19, 46] stated above only work over groups over pp-adic fields FF of charF=0\text{char}\,F=0. Results in positive characteristic are more ad-hoc for specific groups. In his thesis [49], Ray-Dulany proved the base change fundamental lemma for Iwahori-Hecke algebra of GL2\mathrm{GL}_{2} for any local field with characteristic not equal to 22 by explicit calculations. In [14], Feng gave a geometric proof of the base change fundamental lemma for regular semisimple elements for parahoric Hecke algebras of GLn\mathrm{GL}_{n} over local function fields using cohomology of certain moduli stacks of shtukas and the Langlands-Kottwitz method, which generalized the previous results by [48] for spherical Hecke algebras for GLn\mathrm{GL}_{n} over local function fields. Most recently, Bartling and Ito[4] prove base change fundamental lemma for central elements in the parahoric Hecke algebras for general unramified reductive groups over local function fields, using the technique of close local fields.

In this article, we prove the base change fundamental lemma for Bernstein centers of depth-zero principal series blocks at regular semisimple elements in unramified groups GG over local function fields, following and generalizing the strategies in [18, 19]. To state the theorem, let us fix some more notations. Denote the ring of integers of FF by 𝒪F\mathcal{O}_{F}. Let AA denote a maximal FF-split torus of GG and set T=ZG(A)T=Z_{G}(A), a maximal torus of GG which is defined and unramified over FF. We can choose an Iwahori subgroup IG(F)I\subset G(F) which is in good position relative to TT. Let I+I^{+} denote the pro-unipotent radical of II. Furthermore, let T(F)1T(F)_{1} denote the maximal compact open subgroup of T(F)T(F), and let T(F)1+=T(F)1I+T(F)^{+}_{1}=T(F)_{1}\cap I^{+} denotes its pro-unipotent radical. We will denote χ\chi to be a character on T(F)1/T(F)1+T(F)_{1}/T(F)^{+}_{1}. Such characters are called depth-zero characters. Via the canonical isomorphism

T(F)1/T(F)1+I/I+T(F)_{1}/T(F)^{+}_{1}\xrightarrow{\sim}I/I^{+}

we see that χ\chi induces a character ρ:=ρχ\rho:=\rho_{\chi} on II, trivial on I+I^{+}. Then we can consider the Hecke algebra (G,ρ)\mathcal{H}(G,\rho) of our study:

(G,ρ):={fCc(G):f(igi)=ρ1(i)f(g)ρ1(i),i,iI,gG},\mathcal{H}(G,\rho):=\{f\in C^{\infty}_{c}(G):f(igi^{\prime})=\rho^{-1}(i)f(g)\rho^{-1}(i^{\prime}),\forall\,i,i^{\prime}\in I,\,\forall g\in G\},

where the convolution is defined using the Haar measure which gives II volume 11. Write 𝒵(G,ρ)\mathcal{Z}(G,\rho) for Z((G,ρ))Z(\mathcal{H}(G,\rho)).

Let Nr:T(Fr)1T(F)1N_{r}:T(F_{r})_{1}\to T(F)_{1} denote the naive norm homomorphism. Therefore, the character χr:=χNr\chi_{r}:=\chi\circ N_{r} is a depth-zero character on T(Fr)1T(F_{r})_{1}, and it gives rise to the character ρr\rho_{r} on IrI_{r} and the Hecke algebra (Gr,ρr)\mathcal{H}(G_{r},\rho_{r}) with center 𝒵(Gr,ρr)\mathcal{Z}(G_{r},\rho_{r}). Here Gr:=G(Fr)G_{r}:=G(F_{r}) and IrGrI_{r}\subset G_{r} is the Iwahori subgroup corresponding to II.

We will define a base change homomorphism

br:𝒵(Gr,ρr)𝒵(G,ρ)b_{r}:\mathcal{Z}(G_{r},\rho_{r})\to\mathcal{Z}(G,\rho)

Finally we can state the main theorem of this article:

Theorem 1.2.

Let FF be a local function field of arbitrary positive characteristic. Let GG be a connected unramified reductive group defined over FF. Denote Fr/FF_{r}/F to be an unramified extension of local function fields of degree rr. Then for any ϕ𝒵(Gr,ρr)\phi\in\mathcal{Z}(G_{r},\rho_{r}), ϕ\phi and br(ϕ)b_{r}(\phi) have the matching stable orbital integrals at every regular semisimple element.

We write (G(Fr),Ir+)\mathcal{H}(G(F_{r}),I^{+}_{r}) (resp., (G(F),I+)\mathcal{H}(G(F),I^{+}))for the Hecke algebra of locally constant compactly supported functions on G(Fr)G(F_{r}) (resp., G(F)G(F)) that are bi-invariant under the open compact subgroups Ir+I^{+}_{r} (resp., I+I^{+}), the pro-unipotent radical of IrI_{r} (resp., II), and we write 𝒵(G(Fr),Ir+)\mathcal{Z}(G(F_{r}),I^{+}_{r}) (resp., 𝒵(G(F),I+)\mathcal{Z}(G(F),I^{+})) for the center of these Hecke algebras. In [19], §10, a base change homomorphism

br:𝒵(G(Fr),Ir+)𝒵(G(F),I+)b_{r}:\mathcal{Z}(G(F_{r}),I^{+}_{r})\to\mathcal{Z}(G(F),I^{+})

was constructed and characterized using the injection

𝒵(G(Fr),Ir+)χ𝒵(G(Fr),Ir,χ),\mathcal{Z}(G(F_{r}),I^{+}_{r})\hookrightarrow\prod_{\chi^{\prime}}\mathcal{Z}(G(F_{r}),I_{r},\chi^{\prime}),

where χ\chi^{\prime} ranges over the finite set of all depth-zero characters on T(Fr)1T(F_{r})_{1}. As a result, we are able to show a base change fundamental lemma for pro-pp Iwahori subgroups from Theorem 1.2:

Corollary 1.3.

If ϕ𝒵(G(Fr),Ir+)\phi\in\mathcal{Z}(G(F_{r}),I^{+}_{r}), then the functions ϕ\phi and br(ϕ)b_{r}(\phi) are associated.

This article overlaps with [14] in the case when G=GLnG=\mathrm{GL}_{n}. However, we are able to prove the vanishing results when γ\gamma is not a norm, which was not done in loc. cit. Moreover, this article overlaps with [4] for central elements of Iwahori-Hecke algebras, where the results are proved for regular semisimple elements in loc. cit..

1.2. Motivations

The analogs of Theorem 1.2 and Corollary 1.3 for groups over characteristic 00 fields already could be useful in the pseudo-stabilization of the Lefschetz trace formula for certain simple Shimura varieties (see for example, [18], p.4 and [26], §13). For local function fields, similar counting points formula has been estabilished in [52], Theorem 5.9.2. We will explain how Corollary 1.3 could be used to stabilize the corresponding Lefschetz trace formula on certain moduli space of shtukas.

Let XX be a smooth projective geometrically irreducible curve over 𝔽q\mathbb{F}_{q}, let F=𝔽q(X)F=\mathbb{F}_{q}(X) be the function field of XX. For a closed point xXx\in X, we write FxF_{x} the completion of FF at xx and 𝒪x\mathcal{O}_{x} the corresponding valuation ring. Let 𝔸=𝔸F\mathbb{A}=\mathbb{A}_{F} be the group of adeles of the global field FF. Let GG be a connected reductive group over FF and let 𝒢\mathcal{G} be a parahoric model of GG over XX. We also assume that GxG_{x} is unramified. Fix two distinct closed points xx and \infty in XX. Let KG(𝔸)K\subset G(\mathbb{A}) be a compact open subgroup of the form K=KxKx𝒢(𝒪)K=K_{x}K^{x}\mathcal{G}(\mathcal{O}_{\infty}), where KxK^{x} is a sufficiently small open compact subgroup of G(𝔸,x)G(\mathbb{A}^{\infty,x}) and Kx𝒢(𝒪x)K_{x}\subset\mathcal{G}(\mathcal{O}_{x}) is the pro-pp unipotent radical of some Iwahori subgroup Ix𝒢(𝒪x)I_{x}\subset\mathcal{G}(\mathcal{O}_{x}).

Consider a proper moduli space of shtukas Sht:=Sht𝒢,Ξ,Kμ¯\mathrm{Sht}:=\mathrm{Sht}^{\underline{\mu}}_{\mathcal{G},\Xi,K} with two legs and with one leg fixed, over the local ring Spec𝒪y,\mathrm{Spec}\,\mathcal{O}_{y,\infty^{\prime}} (defined in §4.7 in [52]). We assume that the space satisfies some boundedness condition as in loc. cit.. Let f=fxfxf=f_{x}\otimes f^{x} where fxCc(𝒢(𝒪x))f_{x}\in C^{\infty}_{c}(\mathcal{G}(\mathcal{O}_{x})) and fxCc(G(𝔸x))f^{x}\in C^{\infty}_{c}(G(\mathbb{A}^{x})) where the \infty-component of fxf^{x} is given by the characteristic function of 𝒢(𝒪)\mathcal{G}(\mathcal{O}_{\infty}). The elliptic semisimple part of the alternating sum of the traces of the Hecke operator ff composed with a power σr\sigma^{r} of Frobenius at xx is given by

(1.2.1) tr(σr×f|H(ShtF¯y,,¯))ell,reg=(γ0,γ,δ)|ker1(F,Gγ0)|vol(Gγ0(F)\Gγ0(𝔸)/Ξ)OγG(𝔸x,)(fx,)TOδx,σG(Fxr)(ϕr,x)TOδ,σG(Fr)(ϕr,)\begin{split}\mathrm{tr}&(\sigma^{r}\times f\,|\,H^{*}(\mathrm{Sht}\otimes\overline{F}_{y,\infty^{\prime}},\bar{\mathbb{Q}}_{\ell}))^{\mathrm{ell,reg}}\\ &=\sum_{(\gamma_{0};\gamma,\delta)}|\ker^{1}(F,G_{\gamma_{0}})|\mathrm{vol}(G_{\gamma_{0}}(F)\backslash G_{\gamma_{0}}(\mathbb{A})/\Xi)O^{G(\mathbb{A}^{x,\infty})}_{\gamma}(f^{x,\infty})TO^{G(F_{x^{r}})}_{\delta_{x},\sigma}(\phi_{r,x})TO^{G(F_{\infty^{r}})}_{\delta_{\infty},\sigma}(\phi_{r,\infty})\end{split}

where the sum runs over the so called elliptic Kottwitz triples (γ0,γ,δ)G(F)×G(𝔸x,)×G(Fxr×Fr)(\gamma_{0};\gamma,\delta)\in G(F)\times G(\mathbb{A}^{x,\infty})\times G(F_{x^{r}}\times F_{\infty^{r}}) attached to a fixed point with some vanishing properties. Here FxrF_{x^{r}} is the degree-rr unramified extension of FxF_{x}.

In particular, it is conjectured that we can find the test function ϕr,x\phi^{\prime}_{r,x} (resp. ϕr,\phi^{\prime}_{r,\infty}) inside the center 𝒵(G(Fxr),Kxr)\mathcal{Z}(G(F_{x^{r}}),K_{x^{r}}) (resp. 𝒵(G(Fr),Kr)\mathcal{Z}(G(F_{\infty^{r}}),K_{\infty^{r}})) of the Hecke algebra (G(Fxr),Kxr)\mathcal{H}(G(F_{x^{r}}),K_{x^{r}}) (resp. (G(Fr),Kr)\mathcal{H}(G(F_{\infty^{r}}),K_{\infty^{r}})) with the same stable twisted orbital integral as ϕr,x\phi_{r,x} (resp. ϕr,\phi_{r,\infty}). We may simplify the right hand side to be

(1.2.2) τ(G)γ0SOγG(𝔸x,)(fx,)SOδx,σG(Fxr)(ϕr,x)SOδ,σG(Fr)(ϕr,)\tau(G)\sum_{\gamma_{0}}SO^{G(\mathbb{A}^{x,\infty})}_{\gamma}(f^{x,\infty})SO^{G(F_{x^{r}})}_{\delta_{x},\sigma}(\phi^{\prime}_{r,x})SO^{G(F_{\infty^{r}})}_{\delta_{\infty},\sigma}(\phi^{\prime}_{r,\infty})

At the place xx, by Corollary 1.3, we can write

(1.2.3) SOδx,σG(Fxr)(ϕr,x)=SOγxG(Fx)(br,x(ϕr,x))SO^{G(F_{x^{r}})}_{\delta_{x},\sigma}(\phi^{\prime}_{r,x})=SO^{G(F_{x})}_{\gamma_{x}}(b_{r,x}(\phi^{\prime}_{r,x}))

where br,xb_{r,x} is the base change homomorphism br,x:𝒵(G(Fxr),Kxr)𝒵(G(Fx),Kx)b_{r,x}:\mathcal{Z}(G(F_{x^{r}}),K_{x^{r}})\to\mathcal{Z}(G(F_{x}),K_{x}). Similar base change identity holds for the place \infty from the results in [34] since KK_{\infty} is hyperspecial maximal compact open subgroup.

With the extra assumptions that Sht\mathrm{Sht} has no global endoscopy and that the matching (1.2.3) can be extended to all semisimple elements, we may eventually write (1.2.2) as

(1.2.4) τ(G)γ0SOγG(𝔸)(fx,br,x(ϕr,x)br,(ϕr,)),\tau(G)\sum_{\gamma_{0}}SO^{G(\mathbb{A})}_{\gamma}(f^{x,\infty}b_{r,x}(\phi^{\prime}_{r,x})b_{r,\infty}(\phi^{\prime}_{r,\infty})),

which resembles the geometric side of the (stabilized) global trace formula for the regular action RR of f:=fx,br,x(ϕr,x)br,(ϕr,)f^{\prime}:=f^{x,\infty}b_{r,x}(\phi^{\prime}_{r,x})b_{r,\infty}(\phi^{\prime}_{r,\infty}) on the space L2(G(F)AG\G(𝔸))L^{2}(G(F)A_{G}\backslash G(\mathbb{A})):

(1.2.5) trR(f)=πm(π)trπ(f),\mathrm{tr}\,R(f)=\sum_{\pi}m(\pi)\,\mathrm{tr}\,\pi(f^{\prime}),

where π\pi ranges over irreducible representations of L2(G(F)AG\G(𝔸))L^{2}(G(F)A_{G}\backslash G(\mathbb{A})). Therefore, we can relate the local factor of the zeta function with automorphic representations, eventually the LL-function. (See [26], Cor. 1.4 for more details)

1.3. Outline of the paper

In §2, we will define the abstract norm homomorphism for all semisimple elements in a quasi-split reductive group over FF. This generalizes the classical results of Kottwitz [30] to non-perfect fields, using the results from [24]. The abstract norm homomorphism relates the stable twisted conjugacy classes of G(E)G(E) with stable conjugacy classes of G(F)G(F), providing the ”transfer of conjugacy classes” needed in (1.1.1). In §3, we briefly recall the necessary background for the base change fundamental lemma, including the definitions of Iwahori subgroups, Bernstein center for depth-zero principal series blocks and base change homomorphisms.

The core technical content starts from §4. In order to prove Theorem 1.2, we will reduce the problem to the case that the group has simply connected derived group and the element is strongly regular semisimple both in the adjoint group and the group itself (see 4.10). In order to turn the identities between integrals into identities between traces of certain representations, we have to prove a version of very simple trace formulas (§5), then stabilize them (§6) in order to compare them on different groups. Finally, by producing the local data adapted to our situation (§7.3, 7.4), we are able to reduce to the cases considered in [19]. Using the same technique of Labesse elementary functions, we are finally able to prove the main theorem 1.2.

Acknowledgments

I would like to thank my advisor Thomas Haines for suggesting this topic and his continuous encouragement and interest. I would like to thank Shenghao Li for spotting a mistake in the original reduction steps. I also thank Shin Eui Song for informing me the results of Hamacher-Kim. I would like to thank Peter Dillery and Kazuhiro Ito for helpful discussions. This research was partially supported by NSF grants DMS 2200873.

2. Norm Mapping and Conjugacy Completeness

Let FF be a field of characteristic p>0p>0 (not necessarily perfect). Let GG be a connected reductive group over FF. We fix once for all a separable closure FsF^{\text{s}} of FF inside an algebraic closure F¯\bar{F} of FF, and let Γ=Gal(Fs/F)\Gamma=\text{Gal}(F^{s}/F) be the absolute Galois group. Consider a conjugacy class CC of GG. By conjugacy class we mean the conjugacy class in G(Fs)G(F^{s}) (rather than in G(F¯)G(\bar{F})). We denote Cσ:=σ(C)C^{\sigma}:=\sigma(C) and xσ:=σ(x)x^{\sigma}:=\sigma(x) for any xGx\in G. The conjugacy class CC is defined over FF if and only if Cσ=CC^{\sigma}=C for all σΓ\sigma\in\Gamma, and the conjugacy class of an element xGx\in G is defined over FF if and only if xσx^{\sigma} is conjugate to xx under G(Fs)G(F^{s}) for all σΓ\sigma\in\Gamma.

Let E/FE/F be a cyclic extension of degree rr. We further assume GG to be an unramified connected reductive group over FF, let θGal(E/F)\theta\in\text{Gal}(E/F) be a generator. Let RE/FGER_{E/F}G_{E} denote the Weil restriction of scalars of GE:=G×FEG_{E}:=G\times_{F}E to a group over FF. The automorphism θ\theta of EE determines an FF-automorphism of RE/FGER_{E/F}G_{E} and an automorphism on its FF-points G(E)G(E), which will be also denoted by θ\theta.

Consider the concrete norm Nr:G(E)G(E)N_{r}:G(E)\to G(E) given by

Nrδ=δθ(δ)θr1(δ)N_{r}\delta=\delta\theta(\delta)\dots\theta^{r-1}(\delta)

It is easy to see that the conjugacy class of NrδN_{r}\delta in G(Fs)G(F^{s}) is defined over FF since we can calculate that

θ(Nrδ)=δ1(Nrδ)δ\theta(N_{r}\delta)=\delta^{-1}(N_{r}\delta)\delta

The goal is to define a well-defined abstract norm map.

(2.0.1) 𝒩:{stable θ-conjugacy classes in G(E)}{stable conjugacy classes in G(F)}\mathcal{N}:\{\text{stable }\theta\text{-conjugacy classes in }G(E)\}\to\{\text{stable conjugacy classes in }G(F)\}

To make sense of all that, we will have to define stable θ\theta-conjugacy class first, then we will show that the conjugacy class of NrδN_{r}\delta actually has a rational point over FF.

2.1. Stable Twisted Conjugacy

We follow [30], §5. We assume Gder=GscG_{\rm der}=G_{\rm sc} for the moment, later we will remove this assumption by using the zz-extension of GG.

Let I:=RE/FGEI:=R_{E/F}G_{E}, there is a natural isomorphism IEGE××GEI_{E}\xrightarrow{\sim}G_{E}\times\dots\times G_{E}, with the factors indexed by Gal(E/F)\mathrm{Gal}(E/F). The element θGal(E/F)\theta\in\mathrm{Gal}(E/F) determines an automorphism sAutF(I)s\in\text{Aut}_{F}(I), which takes the form

s:(x1,,xr)(xr,x1,,xr1)s:(x_{1},\dots,x_{r})\mapsto(x_{r},x_{1},\dots,x_{r-1})

on EE-valued points. We can identify GG with IsI^{s} by embedding GG into II diagonally. The composition

G(E)=I(F)I(E)=G(E)××G(E)G(E)=I(F)\to I(E)=G(E)\times\dots\times G(E)

is given by

x(xθr1,,xθ,x).x\mapsto(x^{\theta^{r-1}},\dots,x^{\theta},x).

We can also define the concrete norm map on II by Nx=xsr1xsxNx=x^{s^{r-1}}\dots x^{s}\cdot x. It is defined over FF and it is the same on G(E)=I(F)G(E)=I(F) as the norm map N:G(E)G(E)N:G(E)\to G(E) we defined before. We say that x,yI(Fs)x,y\in I(F^{s}) are FsF^{s}-θ\theta-conjugate if there exists an element gI(Fs)g\in I(F^{s}) such that x=gsygx=g^{-s}yg. We say that x,yG(E)x,y\in G(E) are FsF^{s}-θ\theta-conjugate if they are FsF^{s}-θ\theta-conjugate as elements G(E)=I(F)I(Fs)G(E)=I(F)\subset I(F^{s}).

Lemma 2.1.
  1. (1)

    For g,yI(Fs)g,y\in I(F^{s}), we have N(gsyg)=g1(Ny)gN(g^{-s}yg)=g^{-1}(Ny)g.

  2. (2)

    Let x,yI(Fs)x,y\in I(F^{s}). Then x,yx,y are FsF^{s}-θ\theta-conjugate if and only if Nx,NyNx,Ny are conjugate in I(Fs)I(F^{s}).

  3. (3)

    The embedding GIG\hookrightarrow I induces a Γ=Gal(Fs/F)\Gamma=\mathrm{Gal}(F^{s}/F)-equivariant injection from the set of conjugacy classes in G(Fs)G(F^{s}) to the set of conjugacy classes in I(Fs)I(F^{s}).

Proof.

The calculations of [30], Lemma 5.2 are still valid here. The Γ\Gamma-equivariant part is clear since the embedding GIG\hookrightarrow I is defined over FF. Let x,yG(Fs)x,y\in G(F^{s}), then they embed as (x,,x)(x,\dots,x) and (y,,y)(y,\dots,y) in I(Fs)I(F^{s}). Then it is clear that they are conjugate in I(Fs)I(F^{s}) if and only if they are conjugate in G(Fs)G(F^{s}).

We get an immediate corollary from (b) and (c) of Lemma 2.1 above.

Corollary 2.2.

Let x,yG(E)x,y\in G(E). Then Nx,NyNx,Ny are conjugate in G(Fs)G(F^{s}) if and only if x,yx,y are θ\theta-conjugate by an element in G(Fs)G(F^{s}).

To define stable θ\theta-conjugacy, we have to define θ\theta-centralizers.

Definition 2.3.

For xG(E)=I(F)x\in G(E)=I(F), let Isx={gI:gsxg=x}I_{sx}=\{g\in I:g^{-s}xg=x\}. This group will be called the θ\theta-centralizer of xx.

It is an FF-subgroup of II. Since we have IE=GE××GEI_{E}=G_{E}\times\dots\times G_{E}, where the factors are indexed by elements of Gal(E/F)\mathrm{Gal}(E/F): θr1,,θ,1\theta^{r-1},\dots,\theta,1, let p:IEGEp:I_{E}\to G_{E} be the projection onto the last factor: (x1,,xr)xr(x_{1},\dots,x_{r})\mapsto x_{r}.

Remark 2.4.

Consider the FF-points of IsδI_{s\delta} for δG(E)=I(F)\delta\in G(E)=I(F), this can be given as the FF-point of a connected reductive group as follows:

Isδ(F)={gI(F):gsδg=δ}={gG(E):gθδg=δ}\begin{split}I_{s\delta}(F)&=\{g\in I(F):g^{-s}\delta g=\delta\}\\ &=\{g\in G(E):g^{-\theta}\delta g=\delta\}\end{split}

We will denote by GδθG_{\delta\theta} in the remainder of the sections.

Lemma 2.5.

Let xG(E)x\in G(E). Then the projection pp induces an isomorphism (Isx)E(GE)Nx(I_{sx})_{E}\xrightarrow{\sim}(G_{E})_{Nx}. This makes IsxI_{sx} an FF-form of the centralizer of NxNx in GG.

Proof.

The proof of Lemma 5.4 in [30] are still valid here. ∎

We define the notion of σ\sigma-(strongly regular) semisimplicity below.

Definition 2.6.

We say that δG(E)\delta\in G(E) is σ\sigma-semisimple, σ\sigma-regular semisimple or σ\sigma-strongly regular semisimple if NδG(E)N\delta\in G(E) is semisimple, regular semisimple or strongly regular semisimple.

We can show that twisted orbital integral converges for σ\sigma-regular semisimple elements. Let ϕ(G,ρ)\phi\in\mathcal{H}(G,\rho) be a function in the depth-zero Hecke algebra, where as before ρ\rho is a character on II, trivial on I+I^{+}. Since ρ\rho is a character on a finite abelian group, it must be unitary. Therefore, |ϕ|(G,I)|\phi|\in\mathcal{H}(G,I), the Hecke algebra of compactly supported bi-invariant functions under II. Using the results of Proposition 5.2 in [4], we see that the twisted orbital integrals of ϕ\phi converge absolutely for σ\sigma-regular semisimple elements.

Let us assume GG is a general quasi-split reductive group defined over FF, we need to define yet another subgroup IsxI^{\circ}_{sx}. We define IsxI^{\circ}_{sx} as the inverse image under the EE-isomorphism p:IsxGNxp:I_{sx}\to G_{Nx} of the subgroup GNxG^{\circ}_{Nx} of GNxG_{Nx}. We will see that IsxI^{\circ}_{sx} is defined over FF in the following lemma. It is clear that Isx=IsxI^{\circ}_{sx}=I_{sx} when GderG_{\text{der}} is simply connected. In general, we consider a zz-extension α:GG\alpha:G^{\prime}\to G, whose definitions are given below. We will also get a corresponding zz-extension γ:II\gamma:I^{\prime}\to I where I=RE/F((G)E)I^{\prime}=R_{E/F}((G^{\prime})_{E}).

Definition 2.7.

Given a connected reductive group GG over FF, we say that a homomorphism α:GG\alpha:G^{\prime}\to G is a zz-extension of GG if

  1. (1)

    GG^{\prime} is also a connected reductive group over FF, whose derived group is simply connected.

  2. (2)

    ker(α)Z(G)\ker(\alpha)\subset Z(G^{\prime}) and is isomorphic to a product of tori of the form RL/F𝔾mR_{L/F}\mathbb{G}_{m}, where each LL is a finite separable extension of FF.

  3. (3)

    α\alpha is surjective.

The existence of zz-extensions is proved in [13] Prop 3.1.

Lemma 2.8.

For any yG(E)y\in G^{\prime}(E) such that α(y)=x\alpha(y)=x, we have γ(Isy)=Isx\gamma(I^{\prime}_{sy})=I^{\circ}_{sx}. In particular, IsxI^{\circ}_{sx} is defined over FF.

Proof.

It is quite easy to see that γ(Isy)Isx\gamma(I^{\prime}_{sy})\subset I_{sx}. Therefore, the composition pγ:(Isy)EGNxp\circ\gamma:(I^{\prime}_{sy})_{E}\to G_{Nx} makes sense. Since IsyI^{\prime}_{sy} is connected, we have p(γ(Isy))GNxp(\gamma(I^{\prime}_{sy}))\subset G^{\circ}_{Nx}, therefore γ(Isy)Isx\gamma(I^{\prime}_{sy})\subset I^{\circ}_{sx}. Conversely, we use the fact that the map α:GNyGNx\alpha:G^{\prime}_{Ny}\to G^{\circ}_{Nx} is surjective, therefore, the pullback to the isomorphic groups γ:IsyIsx\gamma:I^{\prime}_{sy}\to I^{\circ}_{sx} should still be surjective. ∎

Definition 2.9.

We say that x,yG(E)=I(F)x,y\in G(E)=I(F) are stably θ\theta-conjugate if there exists gI(Fs)g\in I(F^{s}) such that gsxg=yg^{-s}xg=y and gτg1Isxg^{\tau}g^{-1}\in I^{\circ}_{sx} for all τΓ\tau\in\Gamma.

Now since x,yG(E)=I(F)x,y\in G(E)=I(F), we have (gsxg)τ=gτsxgτ=gsxg(g^{-s}xg)^{\tau}=g^{-\tau s}xg^{\tau}=g^{-s}xg, hence gτg1Isxg^{\tau}g^{-1}\in I_{sx} for all τΓ\tau\in\Gamma. Therefore stable θ\theta-conjugacy and FsF^{s}-θ\theta-conjugacy coincide whenever Isx=IsxI^{\circ}_{sx}=I_{sx}, in particular whenever GderG_{\text{der}} is simply connected.

We introduce a special kind of zz-extension α:GG\alpha:G^{\prime}\to G.

Definition 2.10.

We will say that the zz-extension α:GG\alpha:G^{\prime}\to G is adapted to EE (or E/FE/F) if the norm map ker(α)(E)ker(α)(F)\ker(\alpha)(E)\to\ker(\alpha)(F) is surjective.

Lemma 2.11.
  1. (1)

    Let GG be a connected quasi-split reductive group. There exists a zz-extension α:GG\alpha:G^{\prime}\to G adapted to EE.

  2. (2)

    Let α:GG\alpha:G^{\prime}\to G be a zz-extension adapted to EE. Then x,yG(E)x,y\in G(E) are stably θ\theta-conjugate if and only if there exist FsF^{s}-θ\theta-conjugate elements x,yG(E)x^{\prime},y^{\prime}\in G^{\prime}(E) such that α(x)=x\alpha(x^{\prime})=x and α(y)=y\alpha(y^{\prime})=y.

Proof.

The proof of Lemma 5.6 [30] can be adapted to the equal characteristic situation. ∎

2.2. Definition of the Norm Homomorphism

To show that for any δG(E)\delta\in G(E), Nr(δ)N_{r}(\delta) is stably conjugate to an element in G(F)G(F), therefore defines a stable conjugacy class in G(F)G(F), we will have to use the classical results from [33] and recent progress from [24]. Denote F˘\breve{F} to be the maximal unramified extension of FF, in particular we have EF˘E\subset\breve{F}.

Proposition 2.12.

Let δG(F˘)\delta\in G(\breve{F}). Then there exists an FF-Levi subgroup MM and a pair (J,u)(J,u) such that

  1. (1)

    JJ is an inner twist of MM;

  2. (2)

    uu is an F˘\breve{F}-isomorphism JF˘MF˘J_{\breve{F}}\xrightarrow{\sim}M_{\breve{F}};

  3. (3)

    u(θ(x))=bθ(u(x))b1u(\theta(x))=b\cdot\theta(u(x))\cdot b^{-1}.

  4. (4)

    The inner twist uu identifies J(F)J(F) with the set

    {gG(F˘):g1δθ(g)=δ}\{g\in G(\breve{F}):g^{-1}\delta\theta(g)=\delta\}
Proof.

This is from [33] Remark 6.5 and 5.2. See also [24], Prop. 6.2. ∎

Now we use Lemma 8.1 from [24].

Lemma 2.13.

Let GG^{*} be a quasi-split reductive group over an infinite field FF with a simply connected derived subgroup, and HH^{*} an FF-subgroup of GG^{*} containing a maximal torus. Let HH be an inner form of HH^{*}, and fix an inner twist HFsHFsH_{F^{s}}\xrightarrow{\sim}H^{*}_{F^{s}}, hence we can view H(F)H(F) as a subgroup of G(Fs)G^{*}(F^{s}).

Then for any semisimple element aH(F)a\in H(F), the G(Fs)G^{*}(F^{s})-conjugacy class of aa contains an element γG(F)\gamma\in G^{*}(F).

Proof.

The proof in [24] relies on their earlier results (Theorem A.1.1) in [23] on the rationality of regular semisimple conjugacy classes, which we will document below. ∎

Lemma 2.14.

Let FF be any field. Let GG be a connected quasi-split reductive group over FF. Let CGC\subset G be a regular semisimple conjugacy class defined over FF. Then there exists an element xG(F)Cx\in G(F)\cap C.

Remark 2.15.

The lemma above, however, does not show that every semisimple conjugacy class has the same property, but it suffices for the purpose of defining the abstract norm map.

Now we consider an element δG(E)\delta\in G(E) and whose concrete norm Nr(δ)N_{r}(\delta) is semisimple. Since δθ(Nrδ)=(Nrδ)δ\delta\,\theta(N_{r}\delta)=(N_{r}\delta)\delta, by the above proposition, with G=GG^{*}=G, H=MH^{*}=M and H=JH=J. We see that NrδH(F)N_{r}\delta\in H(F), and the stable conjugacy class of NrδN_{r}\delta contains an element of G(F)G(F). Combined with Corollary 2.2, this finishes the definition of the abstract norm map 2.0.1 in the case when GderG_{\text{der}} is simply connected.

For the next step, we need to follow the argument after Lemma 5.1 in [30] to define the abstract norm map for all quasi-split reductive groups. To be specific, we find a zz-extension α:GG\alpha:G^{\prime}\to G adapted to EE. Then we can define the abstract norm map on G(E)G^{\prime}(E) by the previous results, and we have the following commutative diagram

G(E){\lx@inpgf@ignorespaces G^{\prime}(E)}G(F)/{\lx@inpgf@ignorespaces G^{\prime}(F)/\sim}G(E){\lx@inpgf@ignorespaces G(E)}G(F)/{\lx@inpgf@ignorespaces G(F)/\sim}𝒩r\scriptstyle{\lx@inpgf@ignorespaces\mathcal{N}_{r}}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}𝒩r\scriptstyle{\lx@inpgf@ignorespaces\mathcal{N}_{r}}

and we claim that there exists a unique homomorphism, still denoted by 𝒩r\mathcal{N}_{r}, mapping stable-θ\theta-conjugate classes in G(E)G(E) to stable conjugate classes in G(F)G(F). Indeed, uniqueness of the map comes from the fact that α:G(E)G(E)\alpha:G^{\prime}(E)\to G(E) is surjective. For existence, we have to show that if x,yG(E)x,y\in G^{\prime}(E) and α(x)=α(y)\alpha(x)=\alpha(y), then α(𝒩r(x))=α(𝒩r(y))\alpha(\mathcal{N}_{r}(x))=\alpha(\mathcal{N}_{r}(y)) as stable classes. We can find zker(α)(E)z\in\ker(\alpha)(E) such that x=yzx=yz. Since ker(α)\ker(\alpha) is central, we have Nr(x)=Nr(y)Nr(z)N_{r}(x)=N_{r}(y)N_{r}(z) with Nr(z)ker(α)(F)N_{r}(z)\in\ker(\alpha)(F). Hence α(Nr(x))=α(Nr(y))\alpha(N_{r}(x))=\alpha(N_{r}(y)) as desired.

Next, we show that the definition of 𝒩r\mathcal{N}_{r} does not depend on the choice of the zz-extension. As in the [30], this reduces to show that the following diagram is commutative

G1(E){\lx@inpgf@ignorespaces G_{1}(E)}G1(F)/{\lx@inpgf@ignorespaces G_{1}(F)/\sim}G2(E){\lx@inpgf@ignorespaces G_{2}(E)}G2(F)/{\lx@inpgf@ignorespaces G_{2}(F)/\sim}𝒩r\scriptstyle{\lx@inpgf@ignorespaces\mathcal{N}_{r}}𝒩r\scriptstyle{\lx@inpgf@ignorespaces\mathcal{N}_{r}}

for G1,G2G_{1},G_{2} two zz-extensions of GG. But this comes from the definition of 𝒩r\mathcal{N}_{r} when the derived group is simply connected.

This completes the definition of 𝒩r\mathcal{N}_{r} for all elements in a quasi-split reductive group GG with semisimple norms. We are only left to show the following proposition.

Proposition 2.16.

Let x,yG(E)x,y\in G(E). Then x,yx,y are stably θ\theta-conjugate if and only if 𝒩r(x)=𝒩r(y)\mathcal{N}_{r}(x)=\mathcal{N}_{r}(y).

Proof.

The proof of [30] Proposition 5.7 adapts here. ∎

Although it is not needed in this article, we may extend the definition of the abstract norm map to regular semisimple classes in general connected reductive groups GG over FF, that is, we no longer assume that GG is quasi-split. Following [30], §5, we choose an inner twisting ψ:GG\psi:G\to G^{*}, and we will define a norm mapping 𝒩r\mathcal{N}_{r} from stable θ\theta-conjugacy classes in G(E)G(E) to stable conjugacy classes in G(F)G^{*}(F).

We first assume that Gder=GscG_{\rm der}=G_{\rm sc} We assume that δG(E)\delta\in G(E) such that Nr(δ)N_{r}(\delta) is regular semisimple. As before, the conjugacy class of NrδN_{r}\delta in GG is defined over FF. Consider the conjugacy class CC of the regular semisimple element ψ(Nr(δ))\psi(N_{r}(\delta)) in GG^{*}, we see that τ(C)=C\tau(C)=C for any τGal(Fs/F)\tau\in\mathrm{Gal}(F^{s}/F), therefore CC is defined over FF. Lemma 2.14 tells us that there exists a G(Fs)G^{*}(F^{s})-conjugacy class, or stable conjugacy class in G(F)G(F) consisting of elements that are conjugate to ψ(Nr(δ))\psi(N_{r}(\delta)) in G(Fs)G(F^{s}), moreover, by the first paragraph of the proof of Corollary A.1.2 in [23], this class is unique. We define 𝒩r(δ)\mathcal{N}_{r}(\delta) to be this class.

Using the same idea of zz-extensions as before, we can extend the definition of 𝒩r\mathcal{N}_{r} to general connected reductive groups and prove similar properties as Prop. 2.16. Therefore, we conclude this section by the following:

Conclusion 2.17.

Let GG be a connected reductive group defined over local field FF of characteristic p>0p>0 and let E/FE/F be an unramified extension of degree rr. Fix an inner twisting ψ:GG\psi:G\to G^{*}. For elements δG(E)\delta\in G(E) such that NrδN_{r}\delta is regular semisimple, we can define an injective abstract norm map

𝒩r:{stable θ-conjugacy classes in G(E)}{stable conjugacy classes in G(F)}.\mathcal{N}_{r}:\{\text{stable }\theta\text{-conjugacy classes in }G(E)\}\to\{\text{stable conjugacy classes in }G^{*}(F)\}.

If moreover GG is quasi-split, then for elements δG(E)\delta\in G(E) such that NrδN_{r}\delta is semisimple, we can also define an injective abstract norm map

𝒩r:{stable θ-conjugacy classes in G(E)}{stable conjugacy classes in G(F)}.\mathcal{N}_{r}:\{\text{stable }\theta\text{-conjugacy classes in }G(E)\}\to\{\text{stable conjugacy classes in }G(F)\}.

3. Background

In this section, we briefly introduce and review various objects needed to state Theorem 1.2 for completeness.

3.1. Iwahori subgroups

Let FF denote a nonarchimedean local field of characteristics p0p\geq 0. Let 𝒪F\mathcal{O}_{F} denote the ring of integers in FF, and let ϖ𝒪F\varpi\in\mathcal{O}_{F} be a uniformizer. Let q=pnq=p^{n} denote the cardinality of the residue field of FF. Fix an algebraic closure F¯\overline{F} for FF and a separable closure FsF¯F^{s}\subset\overline{F}, and let LL denote the completion of the maximal unramified extension of FF inside FsF^{s}. Let σAut(L/F)\sigma\in\mathrm{Aut}(L/F) denote the Frobenius automorphism of LL over FF. Let 𝒪L\mathcal{O}_{L} denote the ring of integers in LL. The valuation valF:F×\text{val}_{F}:F^{\times}\to\mathbb{Z} is normalized such that valF(ϖ)=1\text{val}_{F}(\varpi)=1. Define |x|F:=qvalF(x)|x|_{F}:=q^{-\text{val}_{F}(x)} for xF×x\in F^{\times}.

Let GG denote a connected reductive group that is defined and unramified over FF. Let AA denote a maximal FF-split torus in GG and set T:=CentG(A)T:=\text{Cent}_{G}(A), a maximal torus in GG defined over FF and split over LL. We will use the symbol GG to denote the group G(F)G(F) of FF-points.

Let E/FE/F be an unramified extension of degree rr contained in LL. We fix a generator θGal(E/F)\theta\in\mathrm{Gal}(E/F) and we use the same symbol θ\theta to denote the induced automorphisms of groups of EE-points T(E),G(E)T(E),G(E), etc.

We consider the Bruhat-Tits building (G(L))\mathcal{B}(G(L)) (resp., (G)\mathcal{B}(G)) for G(L)G(L) (resp., G(F)G(F)). The Bruhat-Tits buildings associated to the semisimple FF-groups GadG_{\text{ad}} and GderG_{\text{der}} can be canonically identified and are denoted ss(G)\mathcal{B}_{ss}(G). The group G(L)Aut(L/F)G(L)\rtimes\mathrm{Aut}(L/F) (resp., G(F)G(F)) acts on (G(L))\mathcal{B}(G(L)) (resp., (G)\mathcal{B}(G)). Via this action, we can identify (G)\mathcal{B}(G) with the σ\sigma-fixed subset (G(L))σ(G(L))\mathcal{B}(G(L))^{\sigma}\subset\mathcal{B}(G(L)).

Let 𝒜L\mathcal{A}^{L} (resp., 𝒜\mathcal{A}) denote the apartment of (G(L))\mathcal{B}(G(L)) (resp., (G)\mathcal{B}(G)) corresponding to the torus TT (resp., AA). Then 𝒜L\mathcal{A}^{L} (resp., 𝒜\mathcal{A}) is endowed with a family of hyperplanes given by the vanishing of the affine roots Φaff(G,T,L)\Phi_{\text{aff}}(G,T,L) (resp., Φaff(G,A,F)\Phi_{\text{aff}}(G,A,F)). Under the identification (G)=(G(L))σ\mathcal{B}(G)=\mathcal{B}(G(L))^{\sigma}, the apartment 𝒜\mathcal{A} is identified with (𝒜L)σ(\mathcal{A}^{L})^{\sigma}. Moreover, the affine roots Φaff(G,A,F)\Phi_{\text{aff}}(G,A,F) are nonconstant restrictions to 𝒜=(𝒜L)σ\mathcal{A}=(\mathcal{A}^{L})^{\sigma} of the affine roots Φaff(G,T,L)\Phi_{\text{aff}}(G,T,L). These affine roots determine the notions of alcoves, facets and Weyl chambers used throughout this article.

We fix once for all a σ\sigma-invariant alcove 𝐚𝒜L\mathbf{a}\in\mathcal{A}^{L}, moreover, within 𝐚¯\bar{\mathbf{a}} we fix a σ\sigma-invariant facet 𝐚J\mathbf{a}_{J} and a σ\sigma-invariant hyperspecial vertex 𝐚0\mathbf{a}_{0}. Kottwitz defines a functorial surjective homomorphism

κG:G(L)X(Z^(G)I)\kappa_{G}:G(L)\longrightarrow X^{*}(\hat{Z}(G)^{I})

where I=Gal(Ls/L)I=\text{Gal}(L^{s}/L) denotes the inertia group. We denote G(L)1:=kerκGG(L)_{1}:=\ker\kappa_{G} by convention.

Definition 3.1.

A parahoric subgroup of G(L)G(L) associated to an arbitrary facet FF of ss(G(L))\mathcal{B}_{\text{ss}}(G(L)) is a subgroup of the form

KF=Fix(F)G(L)1,K_{F}=\mathrm{Fix}(F)\cap G(L)_{1},

where Fix(F)G(L)\mathrm{Fix}(F)\leq G(L) is the subgroup of elements which fix FF pointwise. An Iwahori subgroup of G(L)G(L) is the parahoric subgroup associated to an alcove of ss(G(L))\mathcal{B}_{\text{ss}}(G(L)). A parahoric subgroup of GG will be a subgroup of GG of the form KFGK_{F}\cap G.

Therefore, the facets 𝐚0,𝐚\mathbf{a}_{0},\mathbf{a} and 𝐚J\mathbf{a}_{J} give rise to parahoric subgroups of G(L)G(L): a hyperspecial maximal parahoric subgroup K(L)K(L), an Iwahori subgroup I(L)I(L) and a general parahoric subgroup J(L)J(L). Moreover, we have that K(L)I(L)J(L)K(L)\supset I(L)\subset J(L). Moreover, since the facets are σ\sigma-invariant, we get the corresponding parahoric subgroups K,IK,I and JJ of G(F)G(F) with similar relations.

Remark 3.2.

This definition is taken from [25], which is different from the classical definition of Bruhat-Tits. However, they are equivalent by Prop. 3 in loc. cit.

Remark 3.3.

When G=TG=T is a torus, then there is exactly one parahoric subgroup KK of T(L)T(L), namely,

K=𝒯0(𝒪L),K=\mathcal{T}^{0}(\mathcal{O}_{L}),

where 𝒯0\mathcal{T}^{0} is the identity component of the Neron model of TT. Moreover, we have T(L)1=𝒯0(𝒪L)T(L)_{1}=\mathcal{T}^{0}(\mathcal{O}_{L}).

3.2. Bernstein center for depth-zero principal series

We keep assuming that GG is an unramified connected reductive group over FF. We denote (G)\mathfrak{R}(G) to be the category of smooth representations of G(F)G(F) on \mathbb{C}-vector spaces. All the representations in this article will be on complex vector spaces. The Bernstein center (G)\mathfrak{Z}(G) of the group GG is defined as the ring of endomorphisms of the identity functor on (G)\mathfrak{R}(G). If GG contains an FF-rational parabolic subgroup PP with FF-Levi factor MM and unipotent radical NN (such that P=MNP=MN), we define the modulus function δP:M(F)>0\delta_{P}:M(F)\to\mathbb{R}_{>0} by

δP(m):=|det(Ad(m);Lie(N(F)))|F,\delta_{P}(m):=|\det(\text{Ad}(m);\text{Lie}(N(F)))|_{F},

where ||F|\cdot|_{F} is the normalized absolute value on FF. For σ(M)\sigma\in\mathfrak{R}(M), we will often consider the normalized induced representation

iPG(σ)=IndP(F)G(F)(δP1/2σ),i^{G}_{P}(\sigma)=\text{Ind}^{G(F)}_{P(F)}(\delta^{1/2}_{P}\sigma),

where δP1/2(m)\delta^{1/2}_{P}(m) means the positive square-root of the positive real number δP(m)\delta_{P}(m). The normalization will preserve unitary representations.

Let TT be a maximal unramified FF-torus, which means that TT splits over an unramified extension of FF. In this case T(F)1=T(F)1T(F)_{1}=T(F)^{1} is the unique maximal compact open subgroup of T(F)T(F) ([39], Lemma 2.5.18).

Let T(F)1T(F)_{1} denote the maximal compact open subgroup of T(F)T(F), and let T(F)1+:=T(F)1I+T(F)^{+}_{1}:=T(F)_{1}\cap I^{+} denote its pro-unipotent radical. Let χ\chi denote a depth-zero character on T(F)1T(F)_{1}, which means that χ\chi factors through the quotient T(F)1/T(F)1+T(F)_{1}/T(F)^{+}_{1}. Let χ~\tilde{\chi} denote any extension of χ\chi to a character χ~:T(F)×\tilde{\chi}:T(F)\to\mathbb{C}^{\times}. Consider the inertial class

𝔰=𝔰χ=[T(F),χ~]G.\mathfrak{s}=\mathfrak{s}_{\chi}=[T(F),\tilde{\chi}]_{G}.

The inertial class 𝔰\mathfrak{s} depends only on the W(F)W(F)-orbit of χ\chi.

Let NN denote the norm homomorphism T(E)T(F)T(E)\to T(F). It maps T(E)1T(F)1T(E)_{1}\to T(F)_{1} and T(E)1+T(F)1+T(E)^{+}_{1}\to T(F)^{+}_{1}. Therefore we will use the same notation to denote the norm map on the quotients N:T(E)1/T(E)1+T(F)1/T(F)1+N:T(E)_{1}/T(E)^{+}_{1}\to T(F)_{1}/T(F)^{+}_{1}.

Let χN:=χN\chi_{N}:=\chi\circ N. This will give a depth-zero character on T(E)1T(E)_{1}. The set of all smooth characters on T(F)T(F) carries a left action under the Weyl group W(F)=NGT(F)/T(F)W(F)=N_{G}T(F)/T(F). Let WχW_{\chi} denote the subgroup of elements in W(F)W(F) which fix χ\chi. Similarly we define WχNW_{\chi_{N}} in the Weyl group W(E)W(E) of G(E)G(E).

Let 𝔰(G)\mathfrak{R}_{\mathfrak{s}}(G) denote the Bernstein component indexed by 𝔰\mathfrak{s}, in other words, this is the full subcategory of (G)\mathfrak{R}(G) whose objects have the property that each of their subquotients is a subquotient of a principal series representation iBG(χ~η)i^{G}_{B}(\tilde{\chi}\eta) for some unramified character η\eta of T(F)T(F). Sometimes we denote 𝔰(G)\mathfrak{R}_{\mathfrak{s}}(G) by χ(G)\mathfrak{R}_{\chi}(G).

Now fix χ\chi and 𝔰=𝔰χ\mathfrak{s}=\mathfrak{s}_{\chi} as above. We have

𝔛𝔰={(T,ξ)G}\mathfrak{X}_{\mathfrak{s}}=\{(T,\xi)_{G}\}

of supercuspidal supports (T,ξ)G(T,\xi)_{G} of irreducible representations π\pi in the category χ(G)\mathfrak{R}_{\chi}(G). This means that π\pi is a subquotient of iBG(ξ)i^{G}_{B}(\xi), where BB is any Borel subgroup of GG containing TT as the Levi factor. Here ξ:T(F)×\xi:T(F)\to\mathbb{C}^{\times} is a smooth character extending some W(F)W(F)-conjugate of χ\chi.

Remark 3.4.

There exists at least one WχW_{\chi}-invariant extension χ~\tilde{\chi} of χ\chi, by using the canonical isomorphism X(T)T(F)/T(F)1X_{*}(T)\xrightarrow{\sim}T(F)/T(F)_{1} given by νϖν\nu\mapsto\varpi^{\nu}, where ϖ\varpi is a choice of uniformizer of FF. Hence the extension χ~ϖ\tilde{\chi}^{\varpi} is defined by the formula

χ~ϖ(ϖνt0)=χ(t0),νX(T),t0T(F)1.\tilde{\chi}^{\varpi}(\varpi^{\nu}t_{0})=\chi(t_{0}),\forall\nu\in X_{*}(T),t_{0}\in T(F)_{1}.

Fix one such extension χ~\tilde{\chi}, we have a bijection

A^/Wχ𝔛𝔰η(T,χ~η)G\begin{split}\hat{A}/W_{\chi}&\xrightarrow{\sim}\mathfrak{X}_{\mathfrak{s}}\\ \eta&\mapsto(T,\tilde{\chi}\eta)_{G}\end{split}

where ηA^\eta\in\hat{A} can be viewed as an unramified character on T(F)T(F) as in [18], Lemma 2.4.2. Up to isomorphism, this structure does not depend on the choice of χ\chi in its W(F)W(F)-orbit, nor on the choice of the extension χ~\tilde{\chi} of χ\chi. We have

𝔛𝔰=Spec([X(A)]Wχ)\mathfrak{X}_{\mathfrak{s}}=\mathrm{Spec}(\mathbb{C}[X_{*}(A)]^{W_{\chi}})

We have a isomorphism I/I+T(F)1/T(F)1+I/I^{+}\xrightarrow{\sim}T(F)_{1}/T(F)^{+}_{1}, hence the depth zero character χ:T(F)1/T(F)1+×\chi:T(F)_{1}/T(F)^{+}_{1}\to\mathbb{C}^{\times} induces

ρ=ρχ:I/I+×.\rho=\rho_{\chi}:I/I^{+}\to\mathbb{C}^{\times}.

We have the following proposition. By definition, (I,ρ)(I,\rho) is a Bushnell-Kutzko type for χ(G)\mathfrak{R}_{\chi}(G) means that an irreducible representation π(G)\pi\in\mathfrak{R}(G) belongs to χ(G)\mathfrak{R}_{\chi}(G) if and only if ρπ|I\rho\subset\pi|_{I}.

Proposition 3.5.

The pair (I,ρ)(I,\rho) is a Bushnell-Kutzko type for χ(G)\mathfrak{R}_{\chi}(G).

Proof.

The proof of Theorem 3.0.2 in [17] works for depth-zero case and any characteristic. ∎

Given Proposition 3.5, the category χ(G)\mathfrak{R}_{\chi}(G) is equivalent to the category of (G,ρ)\mathcal{H}(G,\rho)-modules. ([17], Prop. 2.0.3). Let 𝒵(G,ρ):=Z((G,ρ))\mathcal{Z}(G,\rho):=Z(\mathcal{H}(G,\rho)), this also means that there is a canonical algebra isomorphism

(3.2.1) β:[𝔛𝔰]𝒵(G,ρ),\beta:\mathbb{C}[\mathfrak{X_{\mathfrak{s}}}]\xrightarrow{\sim}\mathcal{Z}(G,\rho),

which can be characterized as follows. For an extension ξ\xi of some WW-conjugate of χ\chi, we consider the space iBG(ξ)ρi^{G}_{B}(\xi)^{\rho} of functions fiBG(ξ)f\in i^{G}_{B}(\xi) such that

f(gi)=f(g)ρ(i)f(gi)=f(g)\rho(i)

for all gGg\in G and iIi\in I. Then

z𝒵(G,ρ) acts on the left on iBG(ξ)ρ by the scalar [β1(z)](ξ),z\in\mathcal{Z}(G,\rho)\text{ acts on the left on }i^{G}_{B}(\xi)^{\rho}\text{ by the scalar }[\beta^{-1}(z)](\xi),

where β1(z)\beta^{-1}(z) is viewed as a regular function on the variety 𝔛𝔰\mathfrak{X}_{\mathfrak{s}} and by ξ\xi we mean the point (T,ξ)G𝔛𝔰(T,\xi)_{G}\in\mathfrak{X}_{\mathfrak{s}}, and the action is convolution of functions on GG with suitable Haar measure.

Remark 3.6.

The fact that β1(z)\beta^{-1}(z) is well-defined as a function on the class (T,ξ)G(T,\xi)_{G} means that [β1(z)](wξ)=[β1(z)](ξ)[\beta^{-1}(z)](\,^{w}\xi)=[\beta^{-1}(z)](\xi) for all wWw\in W. In other words, β1(z)\beta^{-1}(z) is WW-invariant as a function of ξ\xi.

3.3. Base change homomorphism

We fix a depth-zero character χ\chi on T(F)1T(F)_{1}, and let (I,ρ)(I,\rho) be the 𝔰=𝔰χ\mathfrak{s}=\mathfrak{s}_{\chi}-type described above. Let AEA^{E} denote the unique maximal EE-split torus in GG containing AA. It is easy to see that T=ZG(AE)T=Z_{G}(A^{E}). Consider χN:=χN\chi_{N}:=\chi\circ N as a depth-zero character on T(E)1T(E)_{1} and consider the corresponding inertial class 𝔰E:=𝔰χN\mathfrak{s}_{E}:=\mathfrak{s}_{\chi_{N}} for G(E)G(E). Let (IE,ρE)(I_{E},\rho_{E}) denote the 𝔰E\mathfrak{s}_{E}-type associated to the character χN\chi_{N}. We denote the corresponding Hecke algebra and its center by (G(E),ρN)\mathcal{H}(G(E),\rho_{N}) and 𝒵(G(E),ρN)\mathcal{Z}(G(E),\rho_{N}), respectively.

There is a canonical morphism of algebraic varieties

N:𝔛𝔰𝔛𝔰E(T,ξ)G(T(E),ξN)G(E),\begin{split}N^{*}:\mathfrak{X}_{\mathfrak{s}}&\to\mathfrak{X}_{\mathfrak{s}_{E}}\\ (T,\xi)_{G}&\mapsto(T(E),\xi_{N})_{G(E)},\end{split}

where ξ\xi denotes an extension of some W(F)W(F)-conjugate of χ\chi. This induces an algebra homomorphism

(3.3.1) N:[𝔛𝔰E][𝔛𝔰]N:\mathbb{C}[\mathfrak{X}_{\mathfrak{s}_{E}}]\to\mathbb{C}[\mathfrak{X}_{\mathfrak{s}}]

Now we can define the base change homomorphism bE:𝒵(G(E),ρN)𝒵(G,ρ)b_{E}:\mathcal{Z}(G(E),\rho_{N})\to\mathcal{Z}(G,\rho) to be the unique morphism making the following diagram commute:

(3.3.2) [𝔛𝔰E]{\lx@inpgf@ignorespaces\mathbb{C}[\mathfrak{X}_{\mathfrak{s}_{E}}]}𝒵(G(E),ρN){\lx@inpgf@ignorespaces\mathcal{Z}(G(E),\rho_{N})}[𝔛𝔰]{\lx@inpgf@ignorespaces\mathbb{C}[\mathfrak{X}_{\mathfrak{s}}]}𝒵(G,ρ){\lx@inpgf@ignorespaces\mathcal{Z}(G,\rho)}\scriptstyle{\lx@inpgf@ignorespaces\sim}β\scriptstyle{\lx@inpgf@ignorespaces\beta}N\scriptstyle{\lx@inpgf@ignorespaces N}bE\scriptstyle{\lx@inpgf@ignorespaces b_{E}}\scriptstyle{\lx@inpgf@ignorespaces\sim}β\scriptstyle{\lx@inpgf@ignorespaces\beta}

We can interpret the diagram in terms of the actions on principal series to get the following lemma:

Lemma 3.7.

For any character ξ:T(F)×\xi:T(F)\to\mathbb{C}^{\times} which extends some W(F)W(F)-conjugate of χ\chi, define ξN:=ξN\xi_{N}:=\xi\circ N, a character on T(E)T(E) which extends some W(E)W(E)-conjugate of χN\chi_{N}. Let z𝒵(G(E),ρE)z\in\mathcal{Z}(G(E),\rho_{E}). Then b(z)b(z) is the unique element in 𝒵(G,ρ)\mathcal{Z}(G,\rho) which acts on every module iBG(ξ)ρi^{G}_{B}(\xi)^{\rho} by the same scalar by which zz acts on iB(E)G(E)(ξN)ρNi^{G(E)}_{B(E)}(\xi_{N})^{\rho_{N}}. In other words,

[β1(b(z))](ξ)=[β1(z)](ξN)[\beta^{-1}(b(z))](\xi)=[\beta^{-1}(z)](\xi_{N})

We can rephrase the above lemma in terms of right actions: for z𝒵(G(E),ρE)z\in\mathcal{Z}(G(E),\rho_{E}), b(z)b(z) acts on the right on iBG(ξ1)ρ1i^{G}_{B}(\xi^{-1})^{\rho^{-1}} by the scalar by which zz acts on the right on iB(E)G(E)(ξN1)ρN1i^{G(E)}_{B(E)}(\xi^{-1}_{N})^{\rho^{-1}_{N}}, in other words,

(3.3.3) chξ1(b(z))=chξN1(z).ch_{\xi^{-1}}(b(z))=ch_{\xi^{-1}_{N}}(z).

We fix wW(F)w\in W(F) and use the same symbol to denote its lift in NG(T)N_{G}(T). The character χw{}^{w}\chi is defined by χw(t)=χ(w1tw){}^{w}\chi(t)=\chi(w^{-1}tw). Similarly, for any suitable function Φ\Phi, we define Φw()=Φ(w1w){}^{w}\Phi(\cdot)=\Phi(w^{-1}\cdot w). We write Iw:=wIw1{}^{w}I:=wIw^{-1} and I+w:=wI+w1{}^{w}I^{+}:=wI^{+}w^{-1}. We extend χw{}^{w}\chi to the character wρ:wI/wI+×{}^{w}\rho:\,^{w}I/^{w}I^{+}\to\mathbb{C}^{\times} using Iwasawa decomposition of Iw{}^{w}I, and therefore we have ρw(wiw1)=ρ(i){}^{w}\rho(wiw^{-1})=\rho(i) for iIi\in I. There is also an isomorphism of algebras (G,I,ρ)(G,wI,wρ)\mathcal{H}(G,I,\rho)\xrightarrow{\sim}\mathcal{H}(G,\,^{w}I,\,^{w}\rho) given by hwhh\mapsto\,^{w}h.

As usual, we let ξ\xi denote an extension of a W(F)W(F)-conjugate of χ\chi. We write Bw:=wBw1{}^{w}B:=wBw^{-1}, then we have an isomorphism

iBG(ξ1)ρ1iBwG(wξ1)ρ1wi^{G}_{B}(\xi^{-1})^{\rho^{-1}}\xrightarrow{\sim}i^{G}_{{}^{w}B}(^{w}\xi^{-1})^{{}^{w}\rho^{-1}}

given by ΨwΨ\Psi\mapsto\,^{w}\Psi. This isomorphism also intertwines the right actions of h(G,I,ρ)h\in\mathcal{H}(G,I,\rho) and hw(G,wI,wρ){}^{w}h\in\mathcal{H}(G,\,^{w}I,\,^{w}\rho), in the sense that

(Ψh)w=wΨwh.{}^{w}(\Psi\cdot h)=\,^{w}\Psi\cdot\,^{w}h.

Taking h=z𝒵(G,I,ρ)h=z\in\mathcal{Z}(G,I,\rho), we have β1(z)(ξ)=β1(wz)(wξ)=β1(wz)(ξ)\beta^{-1}(z)(\xi)=\beta^{-1}(\,^{w}z)(\,^{w}\xi)=\beta^{-1}(\,^{w}z)(\xi). The last equality comes from the Remark 3.6. In other words, we have the following commutative diagram:

[𝔛χ]{\lx@inpgf@ignorespaces\mathbb{C}[\mathfrak{X}_{\chi}]}𝒵(G,I,ρ){\lx@inpgf@ignorespaces\mathcal{Z}(G,I,\rho)}[𝔛χ]{\lx@inpgf@ignorespaces\mathbb{C}[\mathfrak{X}_{\chi}]}𝒵(G,wI,wρ){\lx@inpgf@ignorespaces\mathcal{Z}(G,\,^{w}I,\,^{w}\rho)}\scriptstyle{\lx@inpgf@ignorespaces\sim}β\scriptstyle{\lx@inpgf@ignorespaces\beta}=\scriptstyle{\lx@inpgf@ignorespaces=}zwz\scriptstyle{\lx@inpgf@ignorespaces z\mapsto\,^{w}z}\scriptstyle{\lx@inpgf@ignorespaces\sim}β\scriptstyle{\lx@inpgf@ignorespaces\beta}

Combining this diagram with the diagram (3.3.2) for GG and G(E)G(E) respectively, we have the following lemma, which shows the compatibility of zwzz\mapsto\,^{w}z with the base change homomorphism:

Lemma 3.8.

For any wW(F)w\in W(F), the following diagram is commutative:

𝒵(G(E),ρN){\lx@inpgf@ignorespaces\mathcal{Z}(G(E),\rho_{N})}𝒵(G(E),wρE){\lx@inpgf@ignorespaces\mathcal{Z}(G(E),\,^{w}\rho_{E})}𝒵(G,ρ){\lx@inpgf@ignorespaces\mathcal{Z}(G,\rho)}𝒵(G,wρ){\lx@inpgf@ignorespaces\mathcal{Z}(G,\,^{w}\rho)}zwz\scriptstyle{\lx@inpgf@ignorespaces z\mapsto\,^{w}z}b\scriptstyle{\lx@inpgf@ignorespaces b}b\scriptstyle{\lx@inpgf@ignorespaces b}zwz\scriptstyle{\lx@inpgf@ignorespaces z\mapsto\,^{w}z}

4. Reduction Steps

In this section, we follow closely the reduction steps of [18], §5 and [19], §7 with a few adaptations.

4.1. Definition of stable twisted orbital integral

We still denote GG to be an unramified connected reductive FF-group. Let δG(E)\delta\in G(E) be such

that 𝒩δG(F)\mathcal{N}\delta\in G(F) (as a stable class) is semisimple. Let e(δ):=e(Gδσ)e(\delta):=e(G^{\circ}_{\delta\sigma}) denote the sign attached by Kottwitz [31] to the connected reductive FF-group GδσG^{\circ}_{\delta\sigma}. (There is no assumption on the characteristics of the ground field FF in loc. cit.) And define a(δ)a(\delta) to be the cardinality of the set

ker[H1(F,Gδσ)H1(F,Gδσ)]\ker[H^{1}(F,G^{\circ}_{\delta\sigma})\to H^{1}(F,G_{\delta\sigma})]

Therefore a(δ)=1a(\delta)=1 for those GG’s with simply-connected derived group. Now for any function ϕCc(G(E))\phi\in C^{\infty}_{c}(G(E)), we can define its stable twisted orbital integral by

(4.1.1) SOδσ(ϕ):=δe(δ)a(δ)TOδσ(ϕ)SO_{\delta\sigma}(\phi):=\sum_{\delta^{\prime}}e(\delta^{\prime})\,a(\delta^{\prime})TO_{\delta^{\prime}\sigma}(\phi)

where TOδσ(ϕ)TO_{\delta^{\prime}\sigma}(\phi) is defined in [18] (4.4.1). Here δ\delta^{\prime} ranges over σ\sigma-conjugacy classes in G(E)G(E) which are stably σ\sigma-conjugate to δ\delta. As a special case when E=FE=F and σ=id\sigma=id, we have also defined the stable orbital integral SOγ(f)SO_{\gamma}(f) for a semisimple element γG(F)\gamma\in G(F) and for fCc(G(F))f\in C^{\infty}_{c}(G(F)).

4.2. Vanishing statements for non-norms

Lemma 4.1.

Let ϕ𝒵(G(E),ρr)\phi\in\mathcal{Z}(G(E),\rho_{r}). If γ\gamma is not a norm from G(E)G(E), then SOγ(bϕ)=0SO_{\gamma}(b\phi)=0.

Proof.

Recall that bϕ𝒵(G,ρ)b\phi\in\mathcal{Z}(G,\rho). First we assume γ\gamma is elliptic. We will prove the stronger statement that if γG(F)\gamma^{\prime}\in G(F) is stably conjugate to γ\gamma, then bϕ(g1γg)=0b\phi(g^{-1}\gamma^{\prime}g)=0 for every gG(F)g\in G(F). From this we see that SOγ(bϕ)=0SO_{\gamma}(b\phi)=0.

Consider the canonical map p:GscGp:G_{\text{sc}}\to G and the abelian group Hab0(F,G)=G(F)/p(Gsc(F))H^{0}_{\text{ab}}(F,G)=G(F)/p(G_{\text{sc}}(F)). Proposition 2.5.3 of [44] shows that an elliptic element γ\gamma is a norm from G(E)G(E) if and only if its image p(γ)p(\gamma) in Hab0(F,G)H^{0}_{\text{ab}}(F,G) is a norm. (We notice that Labesse didn’t assume the ground field FF to be of characteristic 00 in CHAPITRE 1 and 2 in loc. cit.) Now the required vanishing follows from the following lemma.

Lemma 4.2.

Let f=bϕf=b\phi for some ϕ𝒵(G(E),ρr)\phi\in\mathcal{Z}(G(E),\rho_{r}). Let xG(F)x\in G(F) be any element such that, for some character η\eta on the group Hab0(F,G)H^{0}_{\text{ab}}(F,G) which is trivial on the norms, we have η(x)1\eta(x)\neq 1. Then f(x)=0f(x)=0.

Proof.

We can view η\eta as a character η:G(F)×\eta:G(F)\to\mathbb{C}^{\times} by pulling back along the quotient map G(F)Hab0(F,G)G(F)\twoheadrightarrow H^{0}_{\text{ab}}(F,G), thus the condition η(x)1\eta(x)\neq 1 makes sense.

Since η\eta vanishes on G(F):=p(Gsc(F))G(F)^{\natural}:=p(G_{\text{sc}}(F)), it is trivial on G(F)1=G(F)T(F)1G(F)_{1}=G(F)^{\natural}\cdot T(F)_{1}, where G(F)1G(F)_{1} is also the kernel of the Kottwitz homomorphism κG:G(F)π1(G)IGal(F˘/F)\kappa_{G}:G(F)\to\pi_{1}(G)^{\mathrm{Gal}(\breve{F}/F)}_{I} (see [39], Definition 2.6.23 and Proposition 11.5.4). Here F˘\breve{F} denotes the maximal unramified extension of FF inside a fixed algebraic closure FsF^{s} and I:=Gal(Fs/F˘)I:=\mathrm{Gal}(F^{s}/\breve{F}), and T(F)1T(F)_{1} is the unique maximal compact subgroup of T(F)T(F). Hence the restriction of η\eta to T(F)T(F) is trivial on T(F)1T(F)_{1}. Thus we have fη(G,ρ)f\eta\in\mathcal{H}(G,\rho). By examining the right convolution action of fηf\eta on iBG(ξ1)ρ1i^{G}_{B}(\xi^{-1})^{\rho^{-1}}, we see that fηZ(G,ρ)f\eta\in Z(G,\rho) (also see the proof of Lemma 4.8), and

(4.2.1) chξ1(fη)=ch(ηξ)1(f).ch_{\xi^{-1}}(f\eta)=ch_{(\eta\xi)^{-1}}(f).

But by (3.3.3), this is

ch(ηrξr)1(ϕ)=chξr1(ϕ)=chξ1(f),ch_{(\eta_{r}\xi_{r})^{-1}}(\phi)=ch_{\xi_{r}^{-1}}(\phi)=ch_{\xi^{-1}}(f),

the first equality holds since ηr:=ηNr\eta_{r}:=\eta\,\circ N_{r} is trivial by assumption. This implies that fη=ff\eta=f since chξ1(fη)=chξ1(f)ch_{\xi^{-1}}(f\eta)=ch_{\xi^{-1}}(f) implies that β1(fη)=β1(f)\beta^{-1}(f\eta)=\beta^{-1}(f). Now we have

f(x)(η(x)1)=0f(x)(\eta(x)-1)=0

for such xx. Since η(x)1\eta(x)\neq 1, we have f(x)=0f(x)=0 as desired. ∎

Now consider x:=g1γgx:=g^{-1}\gamma g. Since it is not a norm by assumptions, there must exist one such character η\eta satisfying the conditions of Lemma 4.2, therefore f(x)=0f(x)=0 as desired. We have proved Lemma 4.1 in the case that γ\gamma is elliptic, in the general case, we can apply the descent formula [18] (4.4.6) to reduce to the elliptic case. ∎

4.3. The case where the derived group is not simply connected

The strategy is the same as in [18], §5.2 and [19] §7.2. Choose a finite unramified extension FFF^{\prime}\supset F, which contains EE and splits GG. Consider a zz-extension of FF-groups adapted to E/FE/F:

1ZH𝑝G1,1\longrightarrow Z\longrightarrow H\overset{p}{\longrightarrow}G\longrightarrow 1,

where ZZ is a finite product of copies of ResF/F𝔾m\mathrm{Res}_{F^{\prime}/F}\mathbb{G}_{m}, Hder=HscH_{\text{der}}=H_{\text{sc}} and pp is surjective on EE- and FF-points since ZZ is an induced torus. Choose an extension of σ\sigma to an element in Gal(F/F)\mathrm{Gal}(F^{\prime}/F), which is still denoted σ\sigma. Let Z(E)1Z(E)_{1} (resp. Z(F)1Z(F)_{1}) denote the maximal compact subgroup of Z(E)Z(E) (resp. Z(F)Z(F)). We endow Z(E)Z(E) (resp. Z(F)Z(F)) with the Haar measure giving Z(E)1Z(E)_{1} (resp. Z(F)1Z(F)_{1}) volume 11. The norm homomorphism N:Z(E)Z(F)N:Z(E)\to Z(F) is surjective and determines a measure-preserving isomorphism

N:Z(E)¯:=(Z(E)/(1σ)(Z(E)))Z(F)N:\overline{Z(E)}:=(Z(E)/(1-\sigma)(Z(E)))\to Z(F)

and N:Z(E)1Z(F)1N:Z(E)_{1}\twoheadrightarrow Z(F)_{1} is surjective. Here we give the compact subgroup (1σ)(Z(E))=(1σ)(Z(E)1)(1-\sigma)(Z(E))=(1-\sigma)(Z(E)_{1}) measure 11.

Let λ:Z(F)×\lambda:Z(F)\to\mathbb{C}^{\times} denote a smooth character, and for fCc(H(F))f\in C^{\infty}_{c}(H(F)), we set

fλ(h):=Z(F)f(hz)λ1(z)𝑑zf_{\lambda}(h):=\int_{Z(F)}f(hz)\lambda^{-1}(z)\,dz

Write λ=1\lambda=1 for the trivial character, then we can show that f1(hz)=f1(h)f_{1}(hz^{\prime})=f_{1}(h) for any hH(F)h\in H(F) and zZ(F)z^{\prime}\in Z(F). Therefore we can view f1f_{1} as an element in Cc(G(F))C^{\infty}_{c}(G(F)), which is denoted f¯\bar{f}. Notice that fλf_{\lambda} is only compactly supported modulo Z(F)Z(F)

We write λN\lambda N for the character λN:Z(E)×\lambda\circ N:Z(E)\to\mathbb{C}^{\times}. The depth-zero character χ\chi on T(F)1T(F)_{1} determines a depth-zero character χH\chi_{H} on TH(F)1T_{H}(F)_{1}, where TH:=p1(T)T_{H}:=p^{-1}(T). Let IHI_{H} be the Iwahori subgroup in HH corresponding to the Iwahori subgroup II in GG, and let ρH:IH×\rho_{H}:I_{H}\to\mathbb{C}^{\times} denote the character constructed from χH\chi_{H} by the isomorphism IH/IH+TH(F)1/TH(F)1+I_{H}/I^{+}_{H}\cong T_{H}(F)_{1}/T_{H}(F)^{+}_{1}. For ϕCc(H(E))\phi\in C^{\infty}_{c}(H(E)), we define analogously the function ϕλN\phi_{\lambda N} by the formula

ϕλN(h):=Z(E)ϕ(hz)λ1(Nz)𝑑z,\phi_{\lambda N}(h):=\int_{Z(E)}\phi(hz)\lambda^{-1}(Nz)\,dz,

and similarly we use ϕ¯\bar{\phi} when viewing ϕ1\phi_{1} as an element Cc(G(E))C^{\infty}_{c}(G(E)). It is straightforward to check that the functions ϕλN\phi_{\lambda N} (resp. fλf_{\lambda}) are transformed by λ1N\lambda^{-1}N (resp. λ1\lambda^{-1}) under Z(E)Z(E) (resp. Z(F)Z(F)). These functions are not longer compactly supported on HH, nonetheless we can show that the (twisted) orbital integrals of fλf_{\lambda} (resp. ϕλN\phi_{\lambda N}) exist at (σ)(\sigma)-semisimple element δ\delta by the following simple calculation:

(4.3.1) TOδσH(ϕλN):=Hδσ\H(E)ϕλN(h1δσ(h))dh¯=HδσZ(E)\H(E)Z(F)\Z(E)ϕλN((vh)1δσ(hv))dvdh¯=vol(Z(F)\Z(E))HδσZ(E)\H(E)ϕλN(h¯1δσ(h¯))dh¯=HδσZ(E)\H(E)ϕλN(h¯1δσ(h¯))dh¯\begin{split}TO^{H}_{\delta\sigma}(\phi_{\lambda N}):&=\int_{H_{\delta\sigma}\backslash H(E)}\phi_{\lambda N}(h^{-1}\delta\sigma(h))\,d\bar{h}\\ &=\int_{H_{\delta\sigma}Z(E)\backslash H(E)}\int_{Z(F)\backslash Z(E)}\phi_{\lambda N}((vh)^{-1}\delta\sigma(hv))\,dv\,d\bar{h}\\ &=\text{vol}(Z(F)\backslash Z(E))\int_{H_{\delta\sigma}Z(E)\backslash H(E)}\phi_{\lambda N}(\bar{h}^{-1}\delta\sigma(\bar{h}))\,d\bar{h}\\ &=\int_{H_{\delta\sigma}Z(E)\backslash H(E)}\phi_{\lambda N}(\bar{h}^{-1}\delta\sigma(\bar{h}))\,d\bar{h}\end{split}

Since Z(F)\Z(E)(1σ)Z(E)Z(F)\backslash Z(E)\cong(1-\sigma)Z(E) which has measure 11 and as a function, ϕλN(δσ())\phi_{\lambda N}(\cdot\,\delta\sigma(\cdot)) is compactly supported modulo Z(E)Z(E), the convergence of the (twisted) orbital integral is shown.

We also have the following useful lemma:

Lemma 4.3.

Assume ϕ(H(E),K~,ρ~H)\phi\in\mathcal{H}(H(E),\tilde{K},\tilde{\rho}_{H}) for some compact open subgroup K~H(E)\tilde{K}\leq H(E) and there exists compact open KGK\leq G and a character ρ:K×\rho:K\to\mathbb{C}^{\times} such that

  • K~(1σ)(Z(E))\tilde{K}\supset(1-\sigma)(Z(E)), and

  • ρ~|K~Z(E)=ρN|K~Z(E)\tilde{\rho}|_{\tilde{K}\cap Z(E)}=\rho\circ N|_{\tilde{K}\cap Z(E)}.

Then we have

ϕλN(h)=Z(E)¯ϕ(hz)λ1(Nz)𝑑z¯\phi_{\lambda N}(h)=\int_{\overline{Z(E)}}\phi(hz)\lambda^{-1}(Nz)\,d\bar{z}
Proof.

We have

ϕλN(h)=Z(E)ϕ(hz)λ1(Nz)𝑑z=Z(E)/(1σ)Z(E)(1σ)Z(E)ϕ(vhz)λ1(N(vz))dvdz¯=Z(E)/(1σ)Z(E)(1σ)Z(E)ϕ(hz)λ1(Nz)dvdz¯=Z(E)¯ϕ(hz)λ1(Nz)dz¯\begin{split}\phi_{\lambda N}(h)&=\int_{Z(E)}\phi(hz)\lambda^{-1}(Nz)\,dz\\ &=\int_{Z(E)/(1-\sigma)Z(E)}\int_{(1-\sigma)Z(E)}\phi(vhz)\lambda^{-1}(N(vz))\,dv\,d\bar{z}\\ &=\int_{Z(E)/(1-\sigma)Z(E)}\int_{(1-\sigma)Z(E)}\phi(hz)\lambda^{-1}(Nz)\,dv\,d\bar{z}\\ &=\int_{\overline{Z(E)}}\phi(hz)\lambda^{-1}(Nz)\,d\bar{z}\end{split}

where the second line is [15] Theorem 2.51, the third line follows from that we can write v=vσ(v1)v=v^{\prime}\sigma(v^{\prime-1}) for some vZ(E)v^{\prime}\in Z(E) so that Nv=1Nv=1 and ϕ(vhz)=ϕ(hz)ρ(Nv)=ϕ(hz)\phi(vhz)=\phi(hz)\rho(Nv)=\phi(hz), and in the last line we use our choice of measure that gives (1σ)Z(E)(1-\sigma)Z(E) volume 11. ∎

Lemma 4.4.

Suppose that ϕ(H(E),K~,ρ~)\phi\in\mathcal{H}(H(E),\tilde{K},\tilde{\rho}) (resp. f(H(F),K,ρ)f\in\mathcal{H}(H(F),K,\rho)) for a compact open subgroup K~H(E)\tilde{K}\subset H(E) and a character ρ~:K~×\tilde{\rho}:\tilde{K}\to\mathbb{C}^{\times} (resp. KHK\subset H and ρ:K×\rho:K\to\mathbb{C}^{\times}) such that

  • N(K~Z(E))=KZ(F)N(\tilde{K}\cap Z(E))=K\cap Z(F),

  • K~(1σ)Z(E)\tilde{K}\supset(1-\sigma)Z(E),

  • ρ~|K~Z(E)=ρN|K~Z(E)\tilde{\rho}|_{\tilde{K}\cap Z(E)}=\rho\circ N|_{\tilde{K}\cap Z(E)}.

We have the following statements:

  1. (1)

    The functions ϕ\phi and ff are associated if and only if ϕλN\phi_{\lambda N} and fλf_{\lambda} are associated for every λ\lambda.

  2. (2)

    In (i) we only need to consider characters λ\lambda such that

    λ|KZ(F)=ρ1|KZ(F).\lambda|_{K\cap Z(F)}=\rho^{-1}|_{K\cap Z(F)}.
  3. (3)

    If ϕ(H(E),ρ~H)\phi\in\mathcal{H}(H(E),\tilde{\rho}_{H}) and f(H(F),ρH)f\in\mathcal{H}(H(F),\rho_{H}), then in (i) we only need to consider characters λ\lambda with λ|Z(F)1=χ1|Z(F)1\lambda|_{Z(F)_{1}}=\chi^{-1}|_{Z(F)_{1}}.

  4. (4)

    The pair (ϕ1,f1)(\phi_{1},f_{1}) are associated if and only if (ϕ¯,f¯)(\bar{\phi},\bar{f}) are associated.

Proof.

We follow the proof of Lemma 5.3.1 in [18]. Suppose that δH(E)\delta\in H(E) (resp. γH(F)\gamma\in H(F)), and we write δ¯:=p(δ)\bar{\delta}:=p(\delta) (resp. γ¯:=p(γ)\bar{\gamma}:=p(\gamma)). We have the following formulas for all χ\chi:

(4.3.2) SOδσH(ϕλN):=δe(δ)TOδσH(ϕλN)=δe(δ)Hδσ\H(E)ϕλN(h1δσ(h))dh¯=δe(δ)Hδσ\H(E)Z(E)¯ϕ(h1(δv)σ(h))λ1(Nv)dvdh¯=Z(E)¯[δe(δ)Hδσ\H(E)ϕ(h1(δv)σ(h))𝑑h¯]λ1(Nv)𝑑v=Z(E)¯λ1(Nv)SOvδ,σH(ϕ)dv.\begin{split}SO^{H}_{\delta\sigma}(\phi_{\lambda N})&:=\sum_{\delta^{\prime}}e(\delta^{\prime})\,TO^{H}_{\delta^{\prime}\sigma}(\phi_{\lambda N})\\ &=\sum_{\delta^{\prime}}e(\delta^{\prime})\,\int_{H_{\delta^{\prime}\sigma}\backslash H(E)}\phi_{\lambda N}(h^{-1}\delta^{\prime}\sigma(h))d\bar{h}\\ &=\sum_{\delta^{\prime}}e(\delta^{\prime})\,\int_{H_{\delta^{\prime}\sigma}\backslash H(E)}\int_{\overline{Z(E)}}\phi(h^{-1}(\delta^{\prime}v)\sigma(h))\,\lambda^{-1}(Nv)dv\,d\bar{h}\\ &=\int_{\overline{Z(E)}}\Bigl[\sum_{\delta^{\prime}}e(\delta^{\prime})\,\int_{H_{\delta^{\prime}\sigma}\backslash H(E)}\phi(h^{-1}(\delta^{\prime}v)\sigma(h))\,d\bar{h}\Bigr]\lambda^{-1}(Nv)dv\\ &=\int_{\overline{Z(E)}}\lambda^{-1}(Nv)\,SO^{H}_{v\delta,\sigma}(\phi)\,dv.\end{split}

and similarly we have

(4.3.3) SOγH(fλ)=Z(F)λ1(z)SOzγH(f)𝑑zSO^{H}_{\gamma}(f_{\lambda})=\int_{Z(F)}\lambda^{-1}(z)\,SO^{H}_{z\gamma}(f)\,dz

Then it is clear that if ϕ\phi and ff are associated, then ϕλN\phi_{\lambda N} and fλf_{\lambda} are associated for every λ\lambda. For the inverse, we apply the Fourier inversion formula to get SOvδ,σH(ϕ)=SOzγH(f)SO^{H}_{v\delta,\sigma}(\phi)=SO^{H}_{z\gamma}(f) for vZ(E)v\in Z(E) and zZ(F)z\in Z(F) such that Nv=zNv=z. (as functions of vv and zz, resp.) In particular, let v=1v=1, we have

(4.3.4) SOδσH(ϕ)=SOγH(f)SO^{H}_{\delta\sigma}(\phi)=SO^{H}_{\gamma}(f)

For (ii), we assume f(H(F),K,ρ)f\in\mathcal{H}(H(F),K,\rho), then for any iKZ(F)i\in K\cap Z(F) and hH(F)h\in H(F), we have

fλ(hi)=Z(F)f(hiz)λ1(z)𝑑z=ρ1(i)fλ(h),\begin{split}f_{\lambda}(hi)&=\int_{Z(F)}f(hiz)\lambda^{-1}(z)\,dz\\ &=\rho^{-1}(i)f_{\lambda}(h),\end{split}

also we have

fλ(hi)=Z(F)f(hiz)λ1(z)𝑑z=λ(i)Z(F)f(hu)λ1(u)du=λ(i)fλ(h)\begin{split}f_{\lambda}(hi)&=\int_{Z(F)}f(hiz)\lambda^{-1}(z)\,dz\\ &=\lambda(i)\int_{Z(F)}f(hu)\lambda^{-1}(u)\,du=\lambda(i)f_{\lambda}(h)\end{split}

Therefore either λ|Z(F)K=ρ1|Z(F)K\lambda|_{Z(F)\cap K}=\rho^{-1}|_{Z(F)\cap K} or fλf_{\lambda} vanishes completely on HH.

Part (iii) follows from part (ii) by taking K=IH,K~=I~HK=I_{H},\tilde{K}=\tilde{I}_{H} and ρ~=ρ~H\tilde{\rho}=\tilde{\rho}_{H}.

Finally, we prove part (iv). For λ=1\lambda=1, we claim that for γ=𝒩δ\gamma=\mathcal{N}\delta, we have

(4.3.5) SOδσH(ϕ1)=SOδ¯σG(ϕ¯)SOγH(f1)=SOγ¯G(f¯)\begin{split}SO^{H}_{\delta\sigma}(\phi_{1})&=SO^{G}_{\bar{\delta}\sigma}(\bar{\phi})\\ SO^{H}_{\gamma}(f_{1})&=SO^{G}_{\bar{\gamma}}(\bar{f})\end{split}

Indeed, we have by definition

SOδσH(ϕ1):=δe(δ)TOδσH(ϕ1)SO^{H}_{\delta\sigma}(\phi_{1}):=\sum_{\delta^{\prime}}e(\delta^{\prime})\,TO^{H}_{\delta^{\prime}\sigma}(\phi_{1})

and

SOδ¯σG(ϕ¯):=δ¯e(δ¯)a(δ¯)TOδ¯σG(ϕ¯)SO^{G}_{\bar{\delta}\sigma}(\bar{\phi}):=\sum_{\bar{\delta^{\prime}}}e(\bar{\delta^{\prime}})\,a(\bar{\delta^{\prime}})TO^{G}_{\bar{\delta^{\prime}}\sigma}(\bar{\phi})

We compare those two equalities term by term. First we notice that p:Hδσ(F)Gδ¯σ(F)p:H_{\delta^{\prime}\sigma}(F)\to G^{\circ}_{\bar{\delta^{\prime}}\sigma}(F) with kernel Z(E)Hδσ(F)=Z(F)Z(E)\cap H_{\delta^{\prime}\sigma}(F)=Z(F), hence e(δ):=e(Hδσ)=e(Gδ¯σ)=:e(δ¯)e(\delta^{\prime}):=e(H_{\delta^{\prime}\sigma})=e(G_{\bar{\delta^{\prime}}\sigma})=:e(\bar{\delta^{\prime}}) by the Corollary on Page 295 of [31]. Recall that a(δ¯):=|ker[H1(F,Gδ¯σ)H1(F,Gδ¯σ)]|a(\bar{\delta^{\prime}}):=|\ker[H^{1}(F,G^{\circ}_{\bar{\delta^{\prime}}\sigma})\to H^{1}(F,G_{\bar{\delta^{\prime}}\sigma})]|. We claim that pp induces a surjective map from the set

{σ-conjugacy classes δH(E) stably σ-conjugate to δ}\{\sigma\text{-conjugacy classes }\delta^{\prime}\in H(E)\text{ stably }\sigma\text{-conjugate to }\delta\}

onto the set

{σ-conjugacy classes δ¯G(E) stably σ-conjugate to δ¯}\{\sigma\text{-conjugacy classes }\bar{\delta^{\prime}}\in G(E)\text{ stably }\sigma\text{-conjugate to }\bar{\delta}\}

with the fiber over the class of δ¯\bar{\delta^{\prime}} identified with the set

ker[H1(F,Gδ¯σ)H1(F,Gδ¯σ)]\ker[H^{1}(F,G^{\circ}_{\bar{\delta^{\prime}}\sigma})\to H^{1}(F,G_{\bar{\delta^{\prime}}\sigma})]

Indeed, we denote G~:=RE/FGE\tilde{G}:=R_{E/F}G_{E}, and similarly H~\tilde{H}. The set of σ\sigma-conjugacy classes in G(E)G(E) which are stably σ\sigma-conjugate to δ¯\bar{\delta} corresponds to the image of

ker[H1(F,Gδ¯σ)H1(F,G~)]\ker[H^{1}(F,G^{\circ}_{\bar{\delta}\sigma})\to H^{1}(F,\tilde{G})]

in

ker[H1(F,Gδ¯σ)H1(F,G~)].\ker[H^{1}(F,G_{\bar{\delta}\sigma})\to H^{1}(F,\tilde{G})].

Meanwhile the set of σ\sigma-conjugacy classes in H(E)H(E) which are stably σ\sigma-conjugate to δ\delta corresponds to the set

ker[H1(F,Hδσ)H1(F,H~)]\ker[H^{1}(F,H_{\delta\sigma})\to H^{1}(F,\tilde{H})]

since Hδσ=HδσH_{\delta\sigma}=H^{\circ}_{\delta\sigma}. This is explained in [30], Pages 805-806. The map pp induces a bijection

ker[H1(F,Hδσ)H1(F,H~)]ker[H1(F,Gδ¯σ)H1(F,G~)].\ker[H^{1}(F,H_{\delta\sigma})\to H^{1}(F,\tilde{H})]\xrightarrow{\sim}\ker[H^{1}(F,G^{\circ}_{\bar{\delta}\sigma})\to H^{1}(F,\tilde{G})].

hence the claim is proved. Finally, we have to show that for all σ\sigma-conjugacy classes δ\delta^{\prime} in the fiber over the class of δ¯\bar{\delta}^{\prime},

TOδσH(ϕ1)=TOδ¯σG(ϕ¯)TO^{H}_{\delta^{\prime}\sigma}(\phi_{1})=TO^{G}_{\bar{\delta^{\prime}}\sigma}(\bar{\phi})

From the calculations in (4.3.1), we have indeed:

TOδσH(ϕ1)=(Z(E)Hδσ)\H(E)ϕ1(h1δσ(h))dh¯=Gδ¯σ\G(E)ϕ¯(g1δ¯σ(g))dg¯=TOδ¯σG(ϕ¯).\begin{split}TO^{H}_{\delta^{\prime}\sigma}(\phi_{1})&=\int_{(Z(E)H_{\delta^{\prime}\sigma})\backslash H(E)}\phi_{1}(h^{-1}\delta^{\prime}\sigma(h))\,d\bar{h}\\ &=\int_{G^{\circ}_{\bar{\delta^{\prime}}\sigma}\backslash G(E)}\bar{\phi}(g^{-1}\bar{\delta^{\prime}}\sigma(g))\,d\bar{g}\\ &=TO^{G}_{\bar{\delta^{\prime}}\sigma}(\bar{\phi}).\end{split}

Where the second equality comes from the fact Z(E)Hδσ=p1(Gδ¯σ)Z(E)H_{\delta^{\prime}\sigma}=p^{-1}(G^{\circ}_{\bar{\delta^{\prime}}\sigma}) and H(E)/Z(E)=G(E)H(E)/Z(E)=G(E) since ZZ is a product of induced tori, by Lemma 5.9 and the following remark. Therefore we have SOδσH(ϕ1)=SOδ¯σG(ϕ¯)SO^{H}_{\delta\sigma}(\phi_{1})=SO^{G}_{\bar{\delta}\sigma}(\bar{\phi}), and similarly SOγH(f1)=SOγ¯G(f¯)SO^{H}_{\gamma}(f_{1})=SO^{G}_{\bar{\gamma}}(\bar{f}) (using the analogous Hγ(F)=p1(Gγ¯)H_{\gamma^{\prime}}(F)=p^{-1}(G^{\circ}_{\bar{\gamma^{\prime}}})), thus (iv) is proved. ∎

Lemma 4.5.

The map ϕϕ¯\phi\mapsto\bar{\phi} determines a surjective homomorphism 𝒵(H(E),ρ~H)𝒵(G(E),ρ~)\mathcal{Z}(H(E),\tilde{\rho}_{H})\to\mathcal{Z}(G(E),\tilde{\rho}). It is compatible with the base change homomorphism in the sense that

b(ϕ¯)=b(ϕ)¯.b(\bar{\phi})=\overline{b(\phi)}.
Proof.

The proof is almost the same as in [18] Lemma 5.3.2, but instead of the Bernstein isomorphism BB there, we use β:[𝔛𝔰EH]𝒵(H(E),ρ~H)\beta:\mathbb{C}[\mathfrak{X}_{\mathfrak{s}^{H}_{E}}]\xrightarrow{\sim}\mathcal{Z}(H(E),\tilde{\rho}_{H}) (also β:[𝔛𝔰E]𝒵(G(E),ρ~)\beta:\mathbb{C}[\mathfrak{X}_{\mathfrak{s}_{E}}]\xrightarrow{\sim}\mathcal{Z}(G(E),\tilde{\rho})). Here 𝔰EH:=𝔰χHN\mathfrak{s}^{H}_{E}:=\mathfrak{s}_{\chi_{H}N}. Recall that ξ:T(F)×\xi:T(F)\to\mathbb{C}^{\times} is a smooth character extending some W(F)W(F)-conjugate of the depth zero character χ:T(F)1×\chi:T(F)_{1}\to\mathbb{C}^{\times}. We can extend ξ\xi to a character ξH\xi_{H} on TH(F)T_{H}(F), which extends χH\chi_{H}. Therefore the morphism of algebraic varieties

p:𝔛𝔰E𝔛𝔰EH(T(E),ξN)G(E)(TH(E),ξHN)H(E),\begin{split}p^{*}:\mathfrak{X}_{\mathfrak{s}_{E}}&\to\mathfrak{X}_{\mathfrak{s}^{H}_{E}}\\ (T(E),\xi_{N})_{G(E)}&\mapsto(T_{H}(E),\xi_{H}\circ N)_{H(E)},\end{split}

gives rise to the homomorphism p:[𝔛𝔰EH][𝔛𝔰E]p:\mathbb{C}[\mathfrak{X}_{\mathfrak{s}^{H}_{E}}]\to\mathbb{C}[\mathfrak{X}_{\mathfrak{s}_{E}}] that we need as in the proof in loc. cit. ∎

4.4. The case where the central character is not unitary

In applying Lemma 4.4(i), we need the following lemma which will enable us to assume that λ\lambda is a unitary character on ZZ. It is not necessarily the case that λ\lambda is unitary in our reduction steps. Nonetheless, we can always twist it by a global character as follows.

Lemma 4.6.

If (π,V)(\pi,V) is any smooth ω\omega-representation of G(F)G(F), then there exists a unique positive real-valued character χ\chi on G(F)G(F) such that the restriction of πχ\pi\otimes\chi to Z(F)Z(F) is unitary, and the restriction of χ\chi to Z(F)1Z(F)_{1} is trivial.

Proof.

This is Lemma 5.2.5 in [6]. We notice that by construction in the proof, χ\chi is trivial on the Iwahori subgroup IGI\subset G. ∎

Lemma 4.7.

Assume ϕ𝒵(H(E),ρ~)\phi\in\mathcal{Z}(H(E),\tilde{\rho}) and let f:=bϕ𝒵(H,ρ)f:=b\phi\in\mathcal{Z}(H,\rho). If ϕλN\phi_{\lambda N} and fλf_{\lambda} are associated for all unitary central characters λ:Z(F)×\lambda:Z(F)\to\mathbb{C}^{\times} and all ϕ𝒵(H(E),ρ~)\phi\in\mathcal{Z}(H(E),\tilde{\rho}), then ϕ\phi and ff are associated.

Proof.

By Lemma 4.4 (i) and (iii), the functions ϕ\phi and ff are associated if ϕλN\phi_{\lambda N} and fλf_{\lambda} are associated for every character λ\lambda such that λ|Z(F)1=χ1|Z(F)1\lambda|_{Z(F)_{1}}=\chi^{-1}|_{Z(F)_{1}}. We claim that it is enough to prove the results for such unitary characters λ\lambda. Indeed, by the previous lemma, we can find positive characters η\eta on GG, such that the set {λη}\{\lambda\eta\} for unitary λ\lambda contains all the characters we need in Lemma 4.4 (i) and (iii).

We consider the function fληf_{\lambda\eta}, where we understand that we actually mean λη|Z\lambda\eta|_{Z} in the definition. Now we have

fλη(g)=Z(F)f(gz)λ1(z)η1(z)𝑑z=η(g)Z(F)f(gz)η1(gz)λ1(z)𝑑z=η(g)(η1f)λ(g).\begin{split}f_{\lambda\eta}(g)&=\int_{Z(F)}f(gz)\lambda^{-1}(z)\eta^{-1}(z)\,dz\\ &=\eta(g)\int_{Z(F)}f(gz)\eta^{-1}(gz)\lambda^{-1}(z)\,dz\\ &=\eta(g)(\eta^{-1}f)_{\lambda}(g).\end{split}

Therefore, we have

(4.4.1) fλη=η(η1f)λ,f_{\lambda\eta}=\eta\cdot(\eta^{-1}f)_{\lambda},

Similarly, we have over H(E)H(E),

(4.4.2) ϕληN=(ηN)((η1N)ϕ)λN\phi_{\lambda\eta N}=(\eta N)\cdot((\eta^{-1}N)\phi)_{\lambda N}

Now we assume ϕ𝒵(H(E),ρ~)\phi\in\mathcal{Z}(H(E),\tilde{\rho}) and f=bϕ𝒵(H,ρ)f=b\phi\in\mathcal{Z}(H,\rho). By the lemma below, η1f\eta^{-1}f and (η1N)ϕ(\eta^{-1}N)\phi are still in the center of respective Hecke algebras and we have b((η1N)ϕ)=η1bϕ=η1fb((\eta^{-1}N)\phi)=\eta^{-1}\cdot b\phi=\eta^{-1}f. Therefore, by assumption, (η1f)λ(\eta^{-1}f)_{\lambda} and ((η1N)ϕ)λN((\eta^{-1}N)\phi)_{\lambda N} are associated. Then by a straightforward calculation, we see that the left hand sides of (4.4.1) and (4.4.2) are associated, as desired. ∎

Lemma 4.8.

Let ϕ𝒵(H(E),ρ)\phi\in\mathcal{Z}(H(E),\rho) and η\eta be a character on HH such that η|I=triv\eta|_{I}=\text{triv}, where IHI\subset H is the Iwahori subgroup where ρ\rho is defined on. Then (ηN)ϕ𝒵(H(E),ρ)(\eta N)\cdot\phi\in\mathcal{Z}(H(E),\rho) and b((ηN)ϕ)=ηbϕb((\eta N)\cdot\phi)=\eta\cdot b\phi.

Proof.

Let ψ(H(E),ρ)\psi\in\mathcal{H}(H(E),\rho). Since η\eta is trivial on II, it is clear that (ηN)ϕ(H(E),ρ)(\eta N)\cdot\phi\in\mathcal{H}(H(E),\rho) then we have

[(ηN)ϕ]ψ(h)=H(E)ηN(g)ϕ(g)ψ(g1h)𝑑g=ηN(h)H(E)ηN(g1)ϕ(hg1)ψ(g)𝑑g=ηN(h)[ϕ((η1N)ψ)](h).\begin{split}[(\eta N)\cdot\phi]\ast\psi(h)&=\int_{H(E)}\eta N(g)\phi(g)\psi(g^{-1}h)\,dg\\ &=\eta N(h)\int_{H(E)}\eta N(g^{-1})\phi(hg^{-1})\psi(g)\,dg\\ &=\eta N(h)[\phi\ast((\eta^{-1}N)\cdot\psi)](h).\end{split}

Therefore we have

[(ηN)ϕ]ψ=ηN[ϕ((η1N)ψ)]=ηN[((η1N)ψ)ϕ](ϕ is central)=ψ[(ηN)ϕ](use the calculation above reversely).\begin{split}[(\eta N)\cdot\phi]\ast\psi&=\eta N\cdot[\phi\ast((\eta^{-1}N)\psi)]\\ &=\eta N\cdot[((\eta^{-1}N)\psi)\ast\phi]\,(\phi\text{ is central})\\ &=\psi\ast[(\eta N)\cdot\phi]\,(\text{use the calculation above reversely}).\end{split}

The centrality is shown. Using the identities (4.2.1) and (3.3.3), we have

chξ1(b((ηN)ϕ))=chξN1((ηN)ϕ)=ch(ξη)N1(ϕ)=ch(ξη)1(bϕ)=chξ1(ηbϕ)\begin{split}ch_{\xi^{-1}}(b((\eta N)\cdot\phi))&=ch_{\xi^{-1}_{N}}((\eta N)\cdot\phi)\\ &=ch_{(\xi\eta)^{-1}_{N}}(\phi)\\ &=ch_{(\xi\eta)^{-1}}(b\phi)\\ &=ch_{\xi^{-1}}(\eta\cdot b\phi)\end{split}

therefore b((ηN)ϕ)=ηbϕb((\eta N)\cdot\phi)=\eta\cdot b\phi, as desired. ∎

4.5. The case where the center is not an induced torus

We assume γG(F)\gamma\in G(F) is a regular elliptic semisimple element, and Gder=GscG_{\text{der}}=G_{\text{sc}}. We will show that there is an exact sequence

1GGQ1,1\longrightarrow G\longrightarrow G^{\prime}\longrightarrow Q\longrightarrow 1,

where GG^{\prime} is an unramified group over FF with the properties that Gder=GscG^{\prime}_{\text{der}}=G^{\prime}_{\text{sc}} and Z(G)Z(G^{\prime}) is an induced torus. We follow the construction in [10], 6.1(b). Indeed, since GG is unramified, Z(G)Z(G) is contained in a maximal unramified FF-torus TGT\subset G. The group of characters X(T)X^{*}(T) is a finitely generated [Gal(F/F)]\mathbb{Z}[\mathrm{Gal}(F^{\prime}/F)]-module, where FF^{\prime} is an unramified extension of FF splitting GG. Let PX(T)P\twoheadrightarrow X^{*}(T) be a free [Gal(F/F)]\mathbb{Z}[\mathrm{Gal}(F^{\prime}/F)]-module. Then dually we get an embedding TZT\hookrightarrow Z^{\prime} where ZZ^{\prime} is an induced torus. We have the following exact sequence

1Z(Gder)Z(G)×GderG1,1\longrightarrow Z(G_{\text{der}})\longrightarrow Z(G)\times G_{\text{der}}\longrightarrow G\longrightarrow 1,

see [47], Example 19.25. We take GG^{\prime} to be (Gder×Z)/Z(Gder)(G_{\text{der}}\times Z^{\prime})/Z(G_{\text{der}}). It is easy to check that Z(G)=ZZ(G^{\prime})=Z^{\prime} and Gder=GderG^{\prime}_{\text{der}}=G_{\text{der}}, therefore GG^{\prime} satisfies the conditions we need.

The natural embedding GGG\hookrightarrow G^{\prime} induces a natural homomorphism

j:𝒵(G,ρ)𝒵(G,ρ)j:\mathcal{Z}(G,\rho)\hookrightarrow\mathcal{Z}(G^{\prime},\rho^{\prime})

by the following commutative diagram

[𝔛𝔰]{\lx@inpgf@ignorespaces\mathbb{C}[\mathfrak{X}_{\mathfrak{s}}]}𝒵(G,ρ){\lx@inpgf@ignorespaces\mathcal{Z}(G,\rho)}[𝔛𝔰]{\lx@inpgf@ignorespaces\mathbb{C}[\mathfrak{X}_{\mathfrak{s}^{\prime}}]}𝒵(G,ρ){\lx@inpgf@ignorespaces\mathcal{Z}(G^{\prime},\rho^{\prime})}\scriptstyle{\lx@inpgf@ignorespaces\sim}β\scriptstyle{\lx@inpgf@ignorespaces\beta}j\scriptstyle{\lx@inpgf@ignorespaces j}\scriptstyle{\lx@inpgf@ignorespaces\sim}β\scriptstyle{\lx@inpgf@ignorespaces\beta}

where the left vertical map is induced by the surjective map

𝔛𝔰𝔛𝔰(T,ξ)G(T:=TG,ξ|T)G\begin{split}\mathfrak{X}_{\mathfrak{s}^{\prime}}&\twoheadrightarrow\mathfrak{X}_{\mathfrak{s}}\\ (T^{\prime},\xi^{\prime})_{G^{\prime}}&\mapsto(T:=T^{\prime}\cap G,\xi^{\prime}|_{T})_{G}\end{split}

where TGT^{\prime}\subset G^{\prime} is a maximal FF-torus and ξ:T(F)×\xi^{\prime}:T^{\prime}(F)\to\mathbb{C}^{\times} is a smooth character extending some W(F)W^{\prime}(F)-conjugate of χ\chi^{\prime}, where WW^{\prime} is the Weyl group of GG^{\prime} and χ:T(F)1×\chi^{\prime}:T^{\prime}(F)_{1}\to\mathbb{C}^{\times} is an extension of χ\chi.

The injective morphism jj is uniquely determined by the Bernstein isomorphisms and it is the restriction of the map between Hecke algebras

(G,ρ)(G,ρ)1nw1nw,\begin{split}\mathcal{H}(G,\rho)&\rightarrow\mathcal{H}(G^{\prime},\rho^{\prime})\\ 1_{n_{w}}&\mapsto 1^{\prime}_{n_{w}},\end{split}

where nwn_{w} is the extended affine Weyl group W~H=X(A)Wχ\tilde{W}_{H}=X_{*}(A)\rtimes W^{\circ}_{\chi} and 1nw1_{n_{w}} (resp. 1nw1^{\prime}_{n_{w}}) is the function in (G,ρ)\mathcal{H}(G,\rho) (resp., (G,ρ)\mathcal{H}(G^{\prime},\rho^{\prime})) supported on IrnwIrI_{r}n_{w}I_{r} (resp., IrnwIrI^{\prime}_{r}n_{w}I^{\prime}_{r}), whose value at nwn_{w} is 11. Such functions 1nw1_{n_{w}} form a basis of the Hecke algebra (G,ρ)\mathcal{H}(G,\rho). Here we are using the notations from §7.3, [19]. Li ([46], Lemma 7.2.3) shows that the morphism jj on the centers is indeed the restriction of the linear transformation on the whole Hecke algebras, therefore, it suffices to prove the following:

Lemma 4.9.

There exists a constant CTC_{T} such that, for every δG(E)\delta\in G(E) with elliptic regular norm in TT, and for every wW~Ew\in\tilde{W}_{E}, we have

(4.5.1) SOδσG(E)(1nw)=CTSOδσG(E)(1nw)SO^{G(E)}_{\delta\sigma}(1_{n_{w}})=C_{T}SO^{G^{\prime}(E)}_{\delta\sigma}(1^{\prime}_{n_{w}})
Proof.

This is proved in [19], Lemma 7.3.1. The proof also works for positive characteristic. ∎

From (4.5.1), we have the following equalities:

(4.5.2) SOγG(f,dt,dg)=cTSOγG(jf,dt,dg)SOδσG(E)(ϕ,dt,dgE)=CTSOδσG(E)(jϕ,dt,dgE),\begin{split}SO^{G}_{\gamma}(f,dt,dg)&=c_{T}SO^{G^{\prime}}_{\gamma}(jf,dt^{\prime},dg^{\prime})\\ SO^{G(E)}_{\delta\sigma}(\phi,dt,dg_{E})&=C_{T}SO^{G^{\prime}(E)}_{\delta\sigma}(j\phi,dt^{\prime},dg_{E}^{\prime}),\end{split}

for all functions f𝒵(G,ρ)f\in\mathcal{Z}(G,\rho) and ϕ𝒵(G(E),ρE)\phi\in\mathcal{Z}(G(E),\rho_{E}) and for all (σ\sigma-)regular (σ\sigma-)elliptic elements γ\gamma and δ\delta in GG whose (σ\sigma-)centralizer is the elliptic FF-torus TT. The proof of Lemma 7.3.1 in loc. cit. shows that the constants cTc_{T} and CTC_{T} making (4.5.2) hold depend only on the torus TT and choices of measures (so not on the functions ff and ϕ\phi, and the choice of γ=𝒩(δ)\gamma=\mathcal{N}(\delta)). Therefore, to force cT=CTc_{T}=C_{T}, we use the fact that 1Ir1_{I_{r}} and 1I1_{I} are associated ([34], §111 1 Kottwitz[34] showed that the functions 1KE1_{K_{E}} and 1K1_{K} are associated for any open bounded subgroup KEK_{E} (resp., KK) of G(E)G(E) (resp., G(F)G(F)) satisfying certain assumptions. In particular, KK (resp. KEK_{E}) satisfies those assumptions when it is the 𝒪F\mathcal{O}_{F}-points (resp. 𝒪E\mathcal{O}_{E}-points) of a smooth and connected affine group scheme over 𝒪F\mathcal{O}_{F} (resp. 𝒪E\mathcal{O}_{E}).) and the stable orbital integrals of 1I1_{I} do not vanish identically on any torus TT in GG.

4.6. Summary of reduction steps

By Lemma 4.1, we may assume that γ\gamma is a norm, and we write γ=𝒩δ\gamma=\mathcal{N}\delta. We assume γ\gamma is regular semisimple from the beginning. Notice that it is different from the assumptions in [18, 19, 10] of just being semisimple since we do not have (twisted) Shalika germs for local function fields and the homogeneity that were used in the proof of Proposition 7.2 in [10] to reduce to regular semisimple elements. The reduction steps (1) and (2) are the same as in [18], 5.4. However, we need to pass it to the global setup afterwards.

  1. (1)

    We may assume that Gder=GscG_{\text{der}}=G_{\text{sc}}. Indeed, for given GG, we take HH to be a zz-extension as in 4.3, and let ϕ𝒵(H(E),ρ~H)\phi\in\mathcal{Z}(H(E),\tilde{\rho}_{H}) with bϕ𝒵(H,ρH)b\phi\in\mathcal{Z}(H,{\rho}_{H}). Assume that (ϕ,bϕ)(\phi,b\phi) are associated, then by Lemma 4.4(i) and (iv), (ϕ¯,bϕ¯)(\overline{\phi},\overline{b\phi}) are associated. By Lemma 4.5, (ϕ¯,bϕ¯)(\bar{\phi},b\bar{\phi}) are associated and ϕ¯\bar{\phi} ranges over all functions in 𝒵(G(E),ρ~)\mathcal{Z}(G(E),\tilde{\rho}), therefore the base change fundamental lemma is proved for GG.

  2. (2)

    We may assume that γ\gamma is elliptic. This is explained in [18], §4 and [19], §6.

    From here we pass to the global setup momentarily. We may assume that GG is split over an unramified extension K/FK/F such that EKE\subset K. We may also assume GG and γ\gamma satisfies the conditions (1) and (2). Choose a degree [K:F][K:F] cyclic extension of function fields K¯/F¯\underline{K}/\underline{F} and a finite place v0v_{0} of F¯\underline{F} such that K¯v0\underline{K}_{v_{0}} is a field and K¯v0/F¯v0K/F\underline{K}_{v_{0}}/\underline{F}_{v_{0}}\cong K/F. Then there is a degree r=[E:F]r=[E:F] cyclic extension E¯/F¯\underline{E}/\underline{F} with E¯K¯\underline{E}\subset\underline{K} and E¯v0/F¯v0E/F\underline{E}_{v_{0}}/\underline{F}_{v_{0}}\cong E/F.

    There is a quasi-split group G¯\underline{G} over F¯\underline{F} with the property that G¯×F¯F¯v0G\underline{G}\times_{\underline{F}}\underline{F}_{v_{0}}\cong G. Let θ\theta denote the F¯\underline{F}-linear automorphism of G¯~\tilde{\underline{G}} from Gal(E/F)Gal(E¯/F¯).\mathrm{Gal}(E/F)\cong\mathrm{Gal}(\underline{E}/\underline{F}).. We may repeat the process of finding a GGG\hookrightarrow G^{\prime} at the beginning of 4.4, but globally: a global group G¯\underline{G^{\prime}} such that G¯der=G¯der\underline{G}^{\prime}_{\text{der}}=\underline{G}_{\text{der}} and Z(G¯)Z(\underline{G}^{\prime}) is an induced torus. Therefore after base change to v0v_{0}, we still have the desired properties for GG and G:=G¯v0G^{\prime}:=\underline{G^{\prime}}_{v_{0}} as in 4.4. Therefore we have the following reduction step:

  3. (3)

    We may assume that Gder=GscG_{\text{der}}=G_{\text{sc}} and Z(G)Z(G) is an induced torus which comes from a global induced torus. Indeed we work under assumptions (1) and (2), and Lemma 4.9 and the discussion there show that we may assume Z(G)Z(G) is indeed an globally induced torus.

  4. (4)

    We may assume that γ\gamma belongs to a specific dense subset in the set of regular elliptic elements. This is explained in [10] Lemma 6.7. Recall that we call a regular semisimple element γ\gamma strongly regular semisimple if GγG_{\gamma} is a (connected) torus. Later in Lemma 5.15, we will see that γG(F)\gamma\in G(F) will be assumed to be strongly regular semisimple, whose image in the adjoint group is still strongly regular. By Lemma 8.7, we will indeed see that such γ\gamma will form a dense subset of the set of regular elliptic elements in G(F)G(F). Notice that we don’t need to worry about the a(δ)a(\delta^{\prime}) terms as in the reduction steps of [18] since our group GG has simply connected derived group.

Conclusion 4.10.

We may assume that Gder=GscG_{\mathrm{der}}=G_{\rm{sc}} with Z(G)Z(G) an globally induced torus, and γ\gamma is a strongly regular elliptic element itself and in the adjoint group, and is a norm.

Remark 4.11.

The reduction steps in [19] have flaws in that Lemma 7.2.3 in loc. cit. is not valid for depth-zero Hecke algebras. Therefore, we cannot reduce to the case that GG is adjoint. The reduction steps here present a solution in order to avoid reducing to adjoint groups.

We hope to show the associations of functions ϕ𝒵(H(E),ρ~)\phi\in\mathcal{Z}(H(E),\tilde{\rho}) and bϕb\phi at all such elements γ\gamma over the group GG. The strategy of the proof in the following sections is that, using Lemma 4.4 (i) and Lemma 4.7, we will show that ϕλN\phi_{\lambda N} and (bϕ)λ(b\phi)_{\lambda} are associated for all unitary central characters and all ϕ𝒵(H(E),ρ~)\phi\in\mathcal{Z}(H(E),\tilde{\rho}), at all strongly regular elliptic semisimple elements in HH whose images in the adjoint group is still strongly regular.

Using the existence of local data adapted to the case with unitary central characters (§7), we are able to show the desired association. In order to produce the adapted local data, one needs to use the global (twisted) trace formulas (§5) and one needs to stabilize the trace formulas (§6) for them to be useful.

5. The Simple Trace Formula

5.1. Setup

This section is mostly independent of other sections. We do not make any assumptions on the characteristics of the global field FF. Our main references for the simple (twisted) trace formula are [1] §1.2 and [12] A.1.

Assume that E/FE/F is a cyclic extension of global fields of degree rr, we write 𝔸\mathbb{A} (resp. 𝔸E\mathbb{A}_{E}) for the adeles of FF (resp. EE). We denote Γ:=Gal(E/F)\Gamma:=\mathrm{Gal}(E/F) and θΓ\theta\in\Gamma be a generator. Let GG be a connected reductive group defined over FF, and let [G]E:=G(E)\G(𝔸E)[G]_{E}:=G(E)\backslash G(\mathbb{A}_{E}) denote the usual adelic quotient over EE. We consider the left action of G(𝔸E)G(\mathbb{A}_{E}) on L2(G(E)\G(𝔸E))L^{2}(G(E)\backslash G(\mathbb{A}_{E})) given by

(5.1.1) (R(g)f)(x):=f(xg)(R(g)f)(x):=f(xg)

for any gG(𝔸E),fL2(G(E)\G(𝔸E))g\in G(\mathbb{A}_{E}),f\in L^{2}(G(E)\backslash G(\mathbb{A}_{E})) and xG(E)\G(𝔸E)x\in G(E)\backslash G(\mathbb{A}_{E}).

Let Z=Z(G)Z=Z(G) be the center of GG. By the reduction steps, we can assume that ZZ is an induced torus over FF, therefore, we have G(R)/Z(R)=Gad(R)G(R)/Z(R)=G_{\rm ad}(R) for any FF-algebra RR, where Gad:=G/ZG_{\rm ad}:=G/Z. Fix a unitary character λ:Z(𝔸F)/Z(F)×\lambda:Z(\mathbb{A}_{F})/Z(F)\to\mathbb{C}^{\times} and define λN:Z(𝔸E)×\lambda N:Z(\mathbb{A}_{E})\to\mathbb{C}^{\times} in the usual way.

We consider the space Cc(Z(𝔸E)\G(𝔸E),λ1)C^{\infty}_{c}(Z(\mathbb{A}_{E})\backslash G(\mathbb{A}_{E}),\lambda^{-1}) of locally constant functions whose supports are compact modulo Z(𝔸E)Z(\mathbb{A}_{E}) and transformed by λ1N\lambda^{-1}N under the action of the center ZZ. We will denote it by Cc(Gad(𝔸E),λ1)C^{\infty}_{c}(G_{\rm ad}(\mathbb{A}_{E}),\lambda^{-1}) with Z(𝔸E)Z(\mathbb{A}_{E}) understood in the definition. Similarly, we consider the space L2(Gad(E)\Gad(𝔸E),λ)=L2(Gad(E)\Gad(𝔸E),λ)L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda)=L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda) of functions on G(E)\G(𝔸E)G(E)\backslash G(\mathbb{A}_{E}) that are square-integrable on Gad(E)\Gad(𝔸E)G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}) which transform by λ\lambda under ZZ. Notice that we need λ\lambda to be unitary in order to define the integrability over the quotient.

Now for any ϕCc(Gad(𝔸E),λ1)\phi\in C^{\infty}_{c}(G_{\rm ad}(\mathbb{A}_{E}),\lambda^{-1}), the above action (5.1.1) induces an action of ϕ\phi on

L2(Gad(E)\Gad(𝔸E),λ),L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda),

given by

(5.1.2) (R(ϕ)f)(x):=Gad(𝔸E)ϕ(g)R(g)f(x)𝑑g=Gad(𝔸E)ϕ(g)f(xg)𝑑g.(R(\phi)f)(x):=\int_{G_{\rm ad}(\mathbb{A}_{E})}\phi(g)R(g)f(x)\,dg=\int_{G_{\rm ad}(\mathbb{A}_{E})}\phi(g)f(xg)\,dg.

for any fL2(Gad(E)\Gad(𝔸E),λ)f\in L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda).

Definition 5.1.

We define the cuspidal subspace

Lcusp2(Gad(E)\Gad(𝔸E),λ)L2(Gad(E)\Gad(𝔸E),λ)L^{2}_{\mathrm{cusp}}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda)\subset L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda)

to be the space of functions ϕL2(Gad(E)\Gad(𝔸E),λ)\phi\in L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda) such that, for every parabolic subgroup PGP\subset G with unipotent radical NN, one has

[N]ϕ(ng)𝑑n=0\int_{[N]}\phi(ng)\,dn=0

for all gG(𝔸E)g\in G(\mathbb{A}_{E}). We call such ϕ\phi cuspidal functions.

We also have the operator

Iθ:L2(Gad(E)\Gad(𝔸E),λ)\displaystyle I_{\theta}:L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda) L2(Gad(E)\Gad(𝔸E),λ),\displaystyle\rightarrow L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda),
f\displaystyle f (xf(θ1(x))),\displaystyle\mapsto(x\mapsto f(\theta^{-1}(x))),

that preserves Lcusp2(Gad(E)\Gad(𝔸E),λ)L^{2}_{\text{cusp}}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda).

Proposition 5.2.

For each ϕCc(Gad(𝔸E),λ1)\phi\in C^{\infty}_{c}(G_{\rm ad}(\mathbb{A}_{E}),\lambda^{-1}), the composite

R(ϕ)Iθ:L2(Gad(E)\Gad(𝔸E),λ)L2(Gad(E)\Gad(𝔸E),λ)R(\phi)\circ I_{\theta}:L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda)\to L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda)

has kernel function

Kϕ(g,θ(h)):=δGad(E)ϕ(g1δθ(h)),K_{\phi}(g,\theta(h)):=\sum_{\delta\in G_{\rm ad}(E)}\phi(g^{-1}\delta\theta(h)),

In other words, we have

(R(ϕ)Iθ(f))(g)=Gad(E)\Gad(𝔸E)Kϕ(g,θ(h))f(h)𝑑h=Gad(E)\Gad(𝔸E)δGad(E)ϕ(g1δθ(h))f(h)𝑑h\begin{split}(R(\phi)\circ I_{\theta}(f))(g)&=\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}K_{\phi}(g,\theta(h))f(h)\,dh\\ &=\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}\sum_{\delta\in G_{\rm ad}(E)}\phi(g^{-1}\delta\theta(h))f(h)\,dh\end{split}

For any fL2(Gad(E)\Gad(𝔸E),λ)f\in L^{2}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda) and gGad(𝔸E)g\in G_{\rm ad}(\mathbb{A}_{E}).

Proof.

Indeed, since

(R(ϕ)Iθ(f))(g)=Gad(𝔸E)ϕ(h)Iθ(f)(gh)dh¯=Gad(𝔸E)ϕ(h)f(θ1(g)θ1(h))dh¯=Gad(𝔸E)ϕ(g1θ(h))f(h)dh¯=Gad(E)\Gad(𝔸E)δGad(E)ϕ(g1δθ(h))f(h)dh¯\begin{split}(R(\phi)\circ I_{\theta}(f))(g)&=\int_{G_{\rm ad}(\mathbb{A}_{E})}\phi(h)I_{\theta}(f)(gh)\,d\bar{h}\\ &=\int_{G_{\rm ad}(\mathbb{A}_{E})}\phi(h)f(\theta^{-1}(g)\theta^{-1}(h))\,d\bar{h}\\ &=\int_{G_{\rm ad}(\mathbb{A}_{E})}\phi(g^{-1}\theta(h))f(h)\,d\bar{h}\\ &=\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}\sum_{\delta\in G_{\rm ad}(E)}\phi(g^{-1}\delta\theta(h))f(h)\,d\bar{h}\end{split}

where the third line follows from change of variables, and the last line follows from a well-known technique called unfolding or integration in stages and the fact that ff is invariant under the action of elements in Gad(E)G_{\rm ad}(E). We also use the fact that the set Gad(E)G_{\rm ad}(E) is θ\theta-stable. For completeness we include the unfolding lemma below. For a proof, see [16] Theorem 3.2.2 and Lemma 9.2.4. ∎

Lemma 5.3.

Suppose that GG is a Hausdorff, locally compact, second countable topological group with right Haar measure dgdg. If fL1(G)f\in L^{1}(G) and ΓG\Gamma\leq G is a discrete subgroup such that the modular character of GG is trivial on Γ\Gamma, then we have

G/ΓγΓf(γg)𝑑g=Gf(g)𝑑g.\int_{G/\Gamma}\sum_{\gamma\in\Gamma}f(\gamma g)\,dg=\int_{G}f(g)\,dg.
Lemma 5.4.

The linear operator Rcusp(ϕ)IθR_{\mathrm{cusp}}(\phi)\circ I_{\theta} is of trace class on Lcusp2(Gad(E)\Gad(𝔸E),λ)L^{2}_{\mathrm{cusp}}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda).

Proof.

Since Rcusp(ϕ):=R(ϕ)|Lcusp2(Gad(E)\Gad(𝔸E),λ)R_{\text{cusp}}(\phi):=R(\phi)|_{L^{2}_{\text{cusp}}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda)} is of trace class by Theorem 9.1.1 of [16], the same is true of Rcusp(ϕ)IθR_{\text{cusp}}(\phi)\circ I_{\theta}, since the set of trace class operators forms a two-sided ideal in the algebra of bounded linear operators on Lcusp2(Gad(E)\Gad(𝔸E),λ)L^{2}_{\text{cusp}}(G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E}),\lambda) (see [11], Lemma 5.3.4). ∎

5.2. Proof of the Simple Trace Formula

Let us choose two places v1,v2v_{1},v_{2} of FF which split completely in EE. We put the following assumptions on the test function ϕCc(Gad(𝔸E),λ1)\phi\in C^{\infty}_{c}(G_{\rm ad}(\mathbb{A}_{E}),\lambda^{-1}):

  1. (1)

    The adelic function ϕ\phi is a (pure) tensor product of local functions ϕ=ϕv\phi=\prod\phi_{v} over places vv of FF, where ϕvCc(G(Ev)/Z(Ev),λ1)\phi_{v}\in C^{\infty}_{c}(G(E_{v})/Z(E_{v}),\lambda^{-1}). For almost all places vv of FF, ϕv\phi_{v} is invariant under G(𝒪Ev)G(\mathcal{O}_{E_{v}}) and supported on Z(Ev)G(𝒪Ev)Z(E_{v})G(\mathcal{O}_{E_{v}}), and satisfies

    Z(Ev)\Z(Ev)G(𝒪Ev)ϕ(g)𝑑g=1.\int_{Z(E_{v})\backslash Z(E_{v})G(\mathcal{O}_{E_{v}})}\phi(g)\,dg=1.
  2. (2)

    On G(Ev1)G(Ew1)×G(Ew2)××G(Ewr)G(E_{v_{1}})\cong G(E_{w_{1}})\times G(E_{w_{2}})\times\dots\times G(E_{w_{r}}), we have ϕv1=(ϕw11,,ϕwr1)\phi_{v_{1}}=(\phi^{1}_{w_{1}},\dots,\phi^{1}_{w_{r}}) where each ϕwi1\phi^{1}_{w_{i}} is a matrix coefficient of the same supercuspidal representation π\pi of G(Ewi)G(Fv1)G(E_{w_{i}})\cong G(F_{v_{1}}). This is possible since by the work of A. Kret[40], we know that supercuspidal representations exist for any reductive group GG over an non-archimedean local field FF. Twisted by a character on the whole group by Lemma 4.6, we may assume that the central character is unitary, and the representation is still supercuspidal since the matrix coefficients are still compactly supported modulo the center.

  3. (3)

    Let ϕv2=(ϕu12,,ϕur2)\phi_{v_{2}}=(\phi^{2}_{u_{1}},\dots,\phi^{2}_{u_{r}}) be the analogous decomposition at v2v_{2}. Let Ωi=Supp(ϕui2)\Omega_{i}=\text{Supp}(\phi^{2}_{u_{i}}), then Ω1Ω2Ωr\Omega_{1}\Omega_{2}\dots\Omega_{r} is contained in the set of elements of G(Fv2)G(F_{v_{2}}) with strongly regular elliptic image in Gad(Fv2)G_{\rm ad}(F_{v_{2}}).

We first show that the assumption (2) implies that the image of R(ϕ)R(\phi) is in the space of cusp forms.

Lemma 5.5.

Let vv be a finite place of EE, let fvCc(G(𝔸Ev))f^{v}\in C^{\infty}_{c}(G(\mathbb{A}^{v}_{E})), and let fvCc(G(Ev))f_{v}\in C^{\infty}_{c}(G(E_{v})) be supercuspidal. Let f(g)=fv(gv)fv(gv)f(g)=f^{v}(g^{v})f_{v}(g_{v}), so that fCc(G(𝔸E))f\in C^{\infty}_{c}(G(\mathbb{A}_{E})). Then R(f)R(f) has cuspidal image.

Recall that we say fvCc(G(Ev))f_{v}\in C^{\infty}_{c}(G(E_{v})) is supercuspidal if

N(Ev)fv(gnh)𝑑n=0,\int_{N(E_{v})}f_{v}(gnh)\,dn=0,

for all proper parabolic subgroup P<GEvP<G_{E_{v}} with unipotent radical NN and for all g,hG(Ev)g,h\in G(E_{v}). As the name suggests, matrix coefficients of supercuspidal representations are indeed supercuspidal, see [16], Lemma 16.4.2.

Proof.

This is standard, for example see Lemma 16.4.1 in [16]. ∎

And we have the main theorem of this section. We define the adelic twisted orbital integral of ϕCc(Gad(𝔸E),λ1)\phi\in C^{\infty}_{c}(G_{\rm ad}(\mathbb{A}_{E}),\lambda^{-1}) to be

TOδθGad(𝔸E)(ϕ)=Gad,δθ(𝔸E)\Gad(𝔸E)ϕ(g1δθ(g))𝑑g.TO^{G_{\rm ad}(\mathbb{A}_{E})}_{\delta\theta}(\phi)=\int_{G_{\rm ad,\delta\theta}(\mathbb{A}_{E})\backslash G_{\rm ad}(\mathbb{A}_{E})}\phi(g^{-1}\delta\theta(g))\,dg.

We notice that the above twisted orbital integral converges since ϕ\phi is compactly supported on Gad(𝔸E)G_{\rm ad}(\mathbb{A}_{E}).

Theorem 5.6.

Under the assumptions (1)(2)(3) above, the operator R(ϕ)R(\phi) sends L2L^{2} automorphic forms into cusp forms, and

(5.2.1) tr(Rcusp(ϕ)Iθ)=δτ(Gad,δθ)TOδθGad(𝔸E)(ϕ)\mathrm{tr}\,(R_{\mathrm{cusp}}(\phi)\circ I_{\theta})=\sum_{\delta}\tau(G_{\rm ad,\delta\theta})TO^{G_{\rm ad}(\mathbb{A}_{E})}_{\delta\theta}(\phi)

where δ\delta runs over the θ\theta-conjugacy classes of elements of Gad(E)G_{\rm ad}(E) with strongly elliptic regular norms, and the group Gad,δθG_{\rm ad,\delta\theta} is the θ\theta-centralizer of δ\delta. Moreover τ(Gad,δθ)=vol(Gad,δθ(E)\Gad,δθ(𝔸E))\tau(G_{\rm ad,\delta\theta})=\text{vol}\,(G_{\rm ad,\delta\theta}(E)\backslash G_{\rm ad,\delta\theta}(\mathbb{A}_{E})).

Proof.

From the lemma above we know that

tr(Rcusp(ϕ)Iθ)=tr(R(ϕ)Iθ)\mathrm{tr}(R_{\text{cusp}}(\phi)\circ I_{\theta})=\mathrm{tr}(R(\phi)\circ I_{\theta})

and we obtain the latter trace by integrating along the diagonal Kϕ(g,θ(g))K_{\phi}(g,\theta(g)) of the kernel associated to R(ϕ)IθR(\phi)\circ I_{\theta}, whence

tr(Rcusp(ϕ)Iθ)=Gad(E)\Gad(𝔸E)Kϕ(g,θ(g))𝑑g=Gad(E)\Gad(𝔸E)δGad(E)ϕ(g1δθ(g))dg.\begin{split}\mathrm{tr}\,(R_{\text{cusp}}(\phi)\circ I_{\theta})&=\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}K_{\phi}(g,\theta(g))\,dg\\ &=\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}\sum_{\delta\in G_{\rm ad}(E)}\phi(g^{-1}\delta\theta(g))dg.\end{split}
Lemma 5.7.

Only those δ\delta with NδN\delta strongly regular elliptic in Gad(E)G_{\rm ad}(E) will appear in the summation above.

Proof.

Same as in [1], P15. ∎

We need to swap the order of the integration and the summation.

Lemma 5.8.

The function

F(g)=δGad(E),Nδstronglyellipticregular|ϕ(g1δθ(g))|F(g)=\sum_{\begin{subarray}{c}\delta\in G_{\rm ad}(E),\\ N\delta\mathrm{\,strongly\,elliptic\,regular}\end{subarray}}|\phi(g^{-1}\delta\theta(g))|

is compactly supported on G(E)Z(𝔸E)\G(𝔸E)G(E)Z(\mathbb{A}_{E})\backslash G(\mathbb{A}_{E}).

Proof.

Using Henniart ([22], Appendice 2), which is valid in positive characteristic, the proof of Lemma 2.6 in [1] adapts. ∎

We regroup the summation by θ\theta-conjugacy by Gad(E)G_{\rm ad}(E):

tr(Rcusp(ϕ)Iθ)=Gad(E)\Gad(𝔸E)δGad(E)Nδ strongly ell. reg.up to Gad(E)-θ-conjugacyδGad(E)δδ by Gad(E)-θ-conjugacyϕ(g1δθ(g))𝑑g,\mathrm{tr}\,(R_{\text{cusp}}(\phi)\circ I_{\theta})=\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}\sum_{\begin{subarray}{c}\delta\in G_{\rm ad}(E)\\ N\delta\text{ strongly ell. reg.}\\ \text{up to }G_{\rm ad}(E)\text{-}\theta\text{-}\text{conjugacy}\end{subarray}}\sum_{\begin{subarray}{c}\delta^{\prime}\in G_{\rm ad}(E)\\ \delta^{\prime}\sim\delta\text{ by }G_{\rm ad}(E)\text{-}\theta\text{-conjugacy}\end{subarray}}\phi(g^{-1}\delta^{\prime}\theta(g))dg,

which implies the final result of the theorem by the following manipulations of integration ”in stages”:

tr(Rcusp(ϕ)Iθ)=δGad(E)\Gad(𝔸E)δGad(E)δδ by Gad(E)-θ-conjugacyϕ(g1δθ(g))𝑑g=δvol(Gad,δθ(E))1Gad(E)\Gad(𝔸E)Gad(E)ϕ(g1v1δθ(v)θ(g))𝑑v𝑑g=δvol(Gad,δθ(E))1Gad(𝔸E)ϕ(g1δθ(g))𝑑g=δvol(Gad,δθ(E))1vol(Gad,δθ(𝔸E))Gad,δθ(𝔸E)\Gad(𝔸E)ϕ(g1δθ(g))𝑑g=δGad(E)Nδ strongly ell. reg.up to Gad(E)-θ-conjugacyvol(Gad,δθ(E)\Gad,δθ(𝔸E))TOδθGad(𝔸E)(ϕ)\begin{split}\mathrm{tr}\,(R_{\text{cusp}}(\phi)\circ I_{\theta})&=\sum_{\delta}\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}\sum_{\begin{subarray}{c}\delta^{\prime}\in G_{\rm ad}(E)\\ \delta^{\prime}\sim\delta\text{ by }G_{\rm ad}(E)\text{-}\theta\text{-conjugacy}\end{subarray}}\phi(g^{-1}\delta^{\prime}\theta(g))dg\\ &=\sum_{\delta}\text{vol}(G_{\rm ad,\delta\theta}(E))^{-1}\int_{G_{\rm ad}(E)\backslash G_{\rm ad}(\mathbb{A}_{E})}\int_{G_{\rm ad}(E)}\phi(g^{-1}v^{-1}\delta\theta(v)\theta(g))\,dv\,dg\\ &=\sum_{\delta}\text{vol}(G_{\rm ad,\delta\theta}(E))^{-1}\int_{G_{\rm ad}(\mathbb{A}_{E})}\phi(g^{-1}\delta\theta(g))dg\\ &=\sum_{\delta}\text{vol}(G_{\rm ad,\delta\theta}(E))^{-1}\,\text{vol}(G_{\rm ad,\delta\theta}(\mathbb{A}_{E}))\int_{G_{\rm ad,\delta\theta}(\mathbb{A}_{E})\backslash G_{\rm ad}(\mathbb{A}_{E})}\phi(g^{-1}\delta\theta(g))dg\\ &=\sum_{\begin{subarray}{c}\delta\in G_{\rm ad}(E)\\ N\delta\text{ strongly ell. reg.}\\ \text{up to }G_{\rm ad}(E)\text{-}\theta\text{-}\text{conjugacy}\end{subarray}}\text{vol}(G_{\rm ad,\delta\theta}(E)\backslash G_{\rm ad,\delta\theta}(\mathbb{A}_{E}))\,TO^{G_{\rm ad}(\mathbb{A}_{E})}_{\delta\theta}(\phi)\end{split}

Thus the theorem is proved. ∎

In the special case of E=FE=F, where r=1r=1 and θ=id\theta=\text{id}, we denote r(f)r(f) to be the representation of fCc(Gad(𝔸),λ1)f\in C^{\infty}_{c}(G_{\rm ad}(\mathbb{A}),\lambda^{-1}) on the space L2(Gad(𝔸),λ)L^{2}(G_{\rm ad}(\mathbb{A}),\lambda), and choose ff similarly as in the twisted case, by the same process, we will have

(5.2.2) tr(rcusp(f))=γτ(Gad,γ)OγGad(𝔸)(f),\mathrm{tr}\,(r_{\text{cusp}}(f))=\sum_{\gamma}\tau(G_{\rm ad,\gamma})O^{G_{\rm ad}(\mathbb{A})}_{\gamma}(f),

where the sum γ\gamma is over the set of conjugacy classes of regular elliptic elements in Gad(F)G_{\rm ad}(F) and τ(Gad,γ):=vol(Gad,γ(F)\Gad,γ(𝔸))\tau(G_{\rm ad,\gamma}):=\text{vol}(G_{\rm ad,\gamma}(F)\backslash G_{\rm ad,\gamma}(\mathbb{A})). Similarly the adelic orbital integral is defined to be

OγGad(𝔸)(f)=Gad,γ(𝔸)\Gad(𝔸)f(g1γg)𝑑gO^{G_{\rm ad}(\mathbb{A})}_{\gamma}(f)=\int_{G_{\rm ad,\gamma}(\mathbb{A})\backslash G_{\rm ad}(\mathbb{A})}f(g^{-1}\gamma g)\,dg

In the next section, we will perform the so-called stabilizations of the trace formulas (5.2.1) and (5.2.2) in order to compare them effectively.

However, before doing that, we will want to examine further the relation between various objects on the group and adjoint group in this setting.

5.3. Passing Between the Adjoint Group and the Group

The trace formulas are given in terms of (twisted) orbital integrals on the adjoint group GadG_{\rm ad}, however, since our functions are defined on GG, later we would like to make statements about integrals on GG. Therefore, it seems necessary to relate various integrals on the group and the adjoint group. In this subsection, we assume that GG is a connected reductive group defined over a local or global field FF with Gder=GscG_{\text{der}}=G_{\text{sc}}. We assume that E/FE/F is a cyclic extension of degree rr, and let θGal(E/F)\theta\in\mathrm{Gal}(E/F) be a generator. We use the same θ\theta to denote the automorphism on the group. We assume that Z(G)Z(G) is an induced torus over FF (in particular, it is connected). We also assume the Haar measure dgdg on G(F)G(F) is normalized so that vol(Z(E)/Z(F))=1\text{vol}(Z(E)/Z(F))=1. Denote Gad:=G/ZG_{\rm ad}:=G/Z, therefore Gad(E)=G(E)/Z(E)G_{\rm ad}(E)=G(E)/Z(E) and Gad(F)=G(F)/Z(F)G_{\rm ad}(F)=G(F)/Z(F).

Assume λ:Z(F)×\lambda:Z(F)\to\mathbb{C}^{\times} is a smooth character trivial on the maximal compact subgroup Z(F)1Z(F)Z(F)_{1}\subset Z(F). Define λN:Z(E)×\lambda N:Z(E)\to\mathbb{C}^{\times} as before, and we still denote it by λ\lambda by abuse of notations. Let ϕCc(Gad(E),λ1)\phi\in C^{\infty}_{c}(G_{\rm ad}(E),\lambda^{-1}) and fCc(Gad(F),λ1)f\in C^{\infty}_{c}(G_{\rm ad}(F),\lambda^{-1}) with similar definitions as in 8.1. Let γG(F)\gamma\in G(F) be a semisimple element. We first prove a technical result:

Lemma 5.9.

The maps Gγ(F)Gad,γ¯(F)G_{\gamma}(F)\to G^{\circ}_{\mathrm{ad},{\bar{\gamma}}}(F) and Gδθ(F)Gad,δ¯θ(F)G_{\delta\theta}(F)\to G^{\circ}_{\mathrm{ad},\bar{\delta}\theta}(F) are surjective.

Proof.

We first notice that it suffices to prove that GγGad,γ¯G_{\gamma}\to G^{\circ}_{\mathrm{ad},\bar{\gamma}} and GδθGad,δ¯θG_{\delta\theta}\to G^{\circ}_{\mathrm{ad},\bar{\delta}\theta} are surjective, as the results over FF-rational point will follow from the long exact sequences induced by

1ZGγGad,γ¯11\longrightarrow Z\longrightarrow G_{\gamma}\longrightarrow G^{\circ}_{\mathrm{ad},\bar{\gamma}}\longrightarrow 1

and

1ZGδθGad,δ¯θ1.1\longrightarrow Z\longrightarrow G_{\delta\theta}\longrightarrow G^{\circ}_{\mathrm{ad},\bar{\delta}\theta}\longrightarrow 1.

We remark that these groups are defined over FF in the second exact sequence. To show that GγGad,γ¯G_{\gamma}\to G^{\circ}_{\mathrm{ad},\bar{\gamma}} is surjective, we notice that GγG_{\gamma} is generated by the maximal torus TT containing γ\gamma and root groups UαU_{\alpha} for roots α\alpha relative to TT such that α(γ)=1\alpha(\gamma)=1. We see that α(γ)=α(γ¯)\alpha(\gamma)=\alpha(\bar{\gamma}) since α(z)=1\alpha(z)=1 for any root α\alpha and zZz\in Z, and TT surjects onto the maximal torus T¯\bar{T} in GadG_{\mathrm{ad}} containing γ\gamma, therefore GγGad,γ¯G_{\gamma}\to G^{\circ}_{\mathrm{ad},\bar{\gamma}} is surjective.

For the twisted centralizers, we have the following commutative diagram:

(Gδθ)E{\lx@inpgf@ignorespaces(G_{\delta\theta})_{E}}(Gad,δ¯θ)E{\lx@inpgf@ignorespaces(G^{\circ}_{\mathrm{ad},\bar{\delta}\theta})_{E}}(GNδ)E{\lx@inpgf@ignorespaces(G_{N\delta})_{E}}(Gad,Nδ¯)E{\lx@inpgf@ignorespaces(G^{\circ}_{\mathrm{ad},N\bar{\delta}})_{E}}\scriptstyle{\lx@inpgf@ignorespaces\simeq}\scriptstyle{\lx@inpgf@ignorespaces\simeq}

therefore, (Gδθ)E(Gad,δ¯θ)E(G_{\delta\theta})_{E}\to(G^{\circ}_{\mathrm{ad},\bar{\delta}\theta})_{E} is a surjection. Since (Gad,δ¯θ)EGad,δ¯θ(G^{\circ}_{\mathrm{ad},\bar{\delta}\theta})_{E}\to G^{\circ}_{\mathrm{ad},\bar{\delta}\theta} is also an FF-surjection , we have GδθGad,δ¯θG_{\delta\theta}\to G^{\circ}_{\mathrm{ad},\bar{\delta}\theta} is surjective, as desired. ∎

Remark 5.10.

In the proof above, it suffices to just assume that ZZ(G)Z\subset Z(G)^{\circ}.

Lemma 5.11.
  1. (1)

    γ\gamma is regular in G(F)G(F) if and only if γ¯\bar{\gamma} is regular in Gad(F)G_{\rm ad}(F);

  2. (2)

    γ\gamma is elliptic in G(F)G(F) if and only if γ¯\bar{\gamma} is elliptic in Gad(F)G_{\rm ad}(F);

  3. (3)

    If γ¯\bar{\gamma} is strongly regular in Gad(F)G_{\rm ad}(F), then so is γ\gamma in G(F)G(F).

Proof.

From the isomorphisms Gγ/ZGad,γ¯G_{\gamma}/Z\cong G^{\circ}_{\rm ad,\bar{\gamma}} and Gγ(F)/Z(F)Gad,γ¯(F)G_{\gamma}(F)/Z(F)\cong G^{\circ}_{\rm ad,\bar{\gamma}}(F), we know that (a)(b) are immediate. (c) also follows since Gγ=GγG_{\gamma}=G^{\circ}_{\gamma} for every semisimple γG(F)\gamma\in G(F). However we don’t even need to assume Gder=GscG_{\text{der}}=G_{\text{sc}}, since Gγ/ZGad,γ¯=Gad,γ¯G_{\gamma}/Z\cong G^{\circ}_{\rm ad,\bar{\gamma}}=G_{\rm ad,\bar{\gamma}}, and since ZZ is connected, GγG_{\gamma} is also connected. ∎

As an easy corollary, let δG(E)\delta\in G(E) be a θ\theta-semisimple element. We have the identity Nδ¯=Nδ¯N\bar{\delta}=\overline{N\delta}. Therefore, we get the same statements by replacing regular (resp., elliptic, strongly regular) with θ\theta-regular (resp., θ\theta-elliptic, θ\theta-strongly regular) and replace γ\gamma (resp. FF) with δ\delta (resp. EE).

Remark 5.12.

We remark that it is not necessary for γ¯\bar{\gamma} to be strongly regular even if γ\gamma is strongly regular. Let FF be a field of characteristic not equal to 22. Consider the matrix

γ=(1001)GL2(F).\gamma=\begin{pmatrix}1&0\\ 0&-1\end{pmatrix}\in\mathrm{GL}_{2}(F).

It is strongly regular semisimple in GL2(F)\mathrm{GL}_{2}(F). However, one can calculate that (PGL2)γ(F)=T(/2)(\mathrm{PGL}_{2})_{\gamma}(F)=T\rtimes(\mathbb{Z}/2\mathbb{Z}), where TT is the one-dimensional maximal split torus consists of diagonal matrices in PGL2\mathrm{PGL}_{2} and the nontrivial element of /2\mathbb{Z}/2\mathbb{Z} is represented by the matrix

(0110).\begin{pmatrix}0&-1\\ 1&0\end{pmatrix}.
Lemma 5.13.

Assume FF is a local field. The projection map π:G(F)Gad(F)\pi:G(F)\to G_{\rm ad}(F) restricts to a surjection

π:{regular elliptic semisimple elements in G(F)}{regular elliptic semisimple elements in Gad(F)}\pi:\{\text{regular elliptic semisimple elements in }G(F)\}\to\{\text{regular elliptic semisimple elements in }G_{\rm ad}(F)\}

Moreover, the inverse image of

{strongly regular elliptic semisimple elements in Gad(F)}\{\text{strongly regular elliptic semisimple elements in }G_{\rm ad}(F)\}

is dense in the left hand side (in the analytic topology22 2 Density in Zariski topology can be similarly shown as in §2.5 in [27], however density in Zariski topology in general does not imply density in analytic topology. of G(F)G(F)).

Proof.

The surjection is from Lemma 5.11(a)(b). Since we have the surjection statement. For the density statement, we fix a maximal FF-torus TT and it is clear that we only to prove the density statement for TT, which follows from the following lemma. ∎

Lemma 5.14.

Let TT be a maximal FF-torus splits over a finite extension. Then the inverse image of

U={strongly regular elliptic elements in Tad(F)}U=\{\text{strongly regular elliptic elements in }T_{\rm ad}(F)\}

is dense in the set of regular elliptic elements in T(F)T(F), in the analytic topology on T(F)T(F).

Proof.

Let X={regular elliptic elements in T(F)}X=\{\text{regular elliptic elements in }T(F)\} and let Y=π1(U)XY=\pi^{-1}(U)\subset X. We claim that X\YX\backslash Y has no interior point in XX, therefore the lemma is proved.

Let W=NG(T)/TW=N_{G}(T)/T absolute Weyl group and let Φ\Phi be the roots relative to TT. Both of them are finite. The condition of yYy\in Y can be described as:

α(y)1 for all αΦw(y)y for all 1wWα(w(y)y1)1 for some αΦ and for all 1wW\begin{split}\alpha(y)&\neq 1\text{ for all }\alpha\in\Phi\\ w(y)&\neq y\text{ for all }1\neq w\in W\\ \alpha(w(y)y^{-1})&\neq 1\text{ for some }\alpha\in\Phi\text{ and for all }1\neq w\in W\end{split}

Therefore, we see that the vanishing locus X\YX\backslash Y is given by a finite number of locally analytic equations. Therefore, locally they are given in terms of a finite number of convergent power series over the non-archimedean field. Therefore they vanish on a set with no interior point, as desired. ∎

Now we can relate orbital integrals on both sides. Assume δG(E)\delta\in G(E) is such that δ¯\bar{\delta} is θ\theta-strongly regular, θ\theta-elliptic and θ\theta-semisimple in Gad(E)G_{\rm ad}(E), and γG(F)\gamma\in G(F) is such that γ¯\bar{\gamma} is strongly regular semisimple in Gad(F)G_{\rm ad}(F).

Lemma 5.15.

We have

(5.3.1) TOδθG(E)(ϕ)=TOδ¯θGad(E)(ϕ)TO^{G(E)}_{\delta\theta}(\phi)=TO^{G_{\rm ad}(E)}_{\bar{\delta}\theta}(\phi)

and

(5.3.2) OγG(F)(f)=Oγ¯Gad(F)(f)O^{G(F)}_{\gamma}(f)=O^{G_{\rm ad}(F)}_{\bar{\gamma}}(f)
Proof.

We will just show the identity (5.3.1), as (5.3.2) follows from the same calculations. Recall that ϕCc(Gad(E),λ1)\phi\in C^{\infty}_{c}(G_{\rm ad}(E),\lambda^{-1}), therefore, the calculation is already done in (4.3.1) given our normalization that vol(Z(E)/Z(F))=1\text{vol}(Z(E)/Z(F))=1. ∎

Lemma 5.16.

Similarly, we have

(5.3.3) SOδθG(E)(ϕ)=SOδ¯θGad(E)(ϕ)SO^{G(E)}_{\delta\theta}(\phi)=SO^{G_{\rm ad}(E)}_{\bar{\delta}\theta}(\phi)

and

(5.3.4) SOγG(F)(f)=SOγ¯Gad(F)(f)SO^{G(F)}_{\gamma}(f)=SO^{G_{\rm ad}(F)}_{\bar{\gamma}}(f)
Proof.

The arguments are exactly like those in the proof of Lemma 4.4 (iv), except it is easier in this case: since δ\delta and δ¯\bar{\delta} are θ\theta-strongly regular, we don’t have the a(δ)a(\delta^{\prime}) terms in the stable orbital integrals. They reduce to

SOδθG(E)(ϕ)=δe(δ)TOδθG(E)(ϕ)SOδ¯θGad(E)(ϕ)=δ¯e(δ¯)TOδ¯θGad(E)(ϕ)\begin{split}SO^{G(E)}_{\delta\theta}(\phi)&=\sum_{\delta^{\prime}}e(\delta^{\prime})TO^{G(E)}_{\delta^{\prime}\theta}(\phi)\\ SO^{G_{\rm ad}(E)}_{\bar{\delta}\theta}(\phi)&=\sum_{\bar{\delta}^{\prime}}e(\bar{\delta}^{\prime})TO^{G_{\rm ad}(E)}_{\bar{\delta}^{\prime}\theta}(\phi)\end{split}

respectly, where δ\delta^{\prime} (resp. δ¯\bar{\delta}^{\prime}) ranges over θ\theta-conjugacy classes in G(E)G(E) (resp. Gad(E)G_{\rm ad}(E)) which are stably θ\theta-conjugate to δ\delta (resp. δ¯\bar{\delta}). The orbital integrals are equal by the previous lemma, and e(δ)=e(δ¯)e(\delta^{\prime})=e(\bar{\delta}^{\prime}) again from [31]. Finally, as in Lemma 4.4 (iv), the surjective map from the set of θ\theta-conjugacy classes in G(E)G(E) which are stably θ\theta-conjugate to δ\delta to the set of θ\theta-conjugacy classes in Gad(E)G_{\rm ad}(E) which are stably θ\theta-conjugate to δ¯\bar{\delta} has single fiber

ker[H1(F,Gad,δ¯θ)H1(F,Gad,δ¯θ)]\ker[H^{1}(F,G^{\circ}_{\rm ad,\bar{\delta}^{\prime}\theta})\to H^{1}(F,G_{\rm ad,\bar{\delta}^{\prime}\theta})]

over δ¯\bar{\delta}^{\prime} since Gad,δ¯θ=Gad,δ¯θG^{\circ}_{\rm ad,\bar{\delta}^{\prime}\theta}=G_{\rm ad,\bar{\delta}^{\prime}\theta} in this case, the lemma is proved. ∎

The upshot of these is that, after stabilization in the next section, we may extract conditional identities of (stable) orbital integrals on GadG_{\rm ad}, but with the relations we have proved in this subsection, we can regard them as identities on GG, which are eventually what we desire.

6. Stabilization of the Twisted Trace Formula

We follow [10], §6.2 closely with some changes along the way.

We fix the notations that will be used in this section. Let E/FE/F be a unramified cyclic extension of global fields of degree rr, and let θGal(E/F)\theta\in\mathrm{Gal}(E/F) be a generator. If GG is an FF-group, then G~:=ResE/FGE\tilde{G}:=\mathrm{Res}_{E/F}G_{E} is the FF-group obtained by the restriction of scalars. We use the same notation θ\theta to denote the FF-linear automorphism of G~\tilde{G} over FF. We denote by 𝔸\mathbb{A} the adeles of FF, and we denote by 𝔸s\mathbb{A}^{s} the ring of adeles of FsF^{s}.

We make the assumption that GG is a quasi-split, connected reductive group over FF, such that GderG_{\text{der}} is simply connected. By the reduction steps, we may also assume that Z(G)Z(G) is an induced torus over FF and let H:=G/Z(G)H:=G/Z(G) to denote the adjoint group in this section, which we denote by GadG_{\rm ad} before, to avoid the overflow of the subscripts. We will assume that HH splits over an unramified extension K/FK/F such that EKE\subset K. We may also assume that H~\tilde{H} satisfies the Hasse principle, that is:

ker1(F,H~):=ker[H1(F,H~)vH1(Fv,H~)]=1.\ker^{1}(F,\tilde{H}):=\ker[H^{1}(F,\tilde{H})\to\prod_{v}H^{1}(F_{v},\tilde{H})]=1.

We denote by 𝒩\mathcal{N} the abstract norm mapping sending regular semisimple elements of H~(F)\tilde{H}(F) to stable conjugacy classes of regular semisimple elements in H(F)H(F), as well as its local versions.

6.1. The Construction of the Obstruction

Let γH(F)\gamma\in H(F) be a strongly regular semisimple element, then its centralizer TT (resp., T~\tilde{T}) is a maximal torus of HH (resp., H~\tilde{H}) over FF. Assume there exists δH~(𝔸)\delta\in\tilde{H}(\mathbb{A}) is such that 𝒩(δv)\mathcal{N}(\delta_{v}) is equal to the stable conjugacy class of γH(Fv)\gamma\in H(F_{v}) for every place vv of FF.

Let NN denote the map xxθ(x)θr1(x)x\mapsto x\theta(x)\dots\theta^{r-1}(x) from H~\tilde{H} to itself. The map N:T~(Fs)T(Fs)N:\tilde{T}(F^{s})\to T(F^{s}) is surjective, so we can choose tT~(Fs)t\in\tilde{T}(F^{s}) such that Nt=γNt=\gamma. Since 𝒩(δv)=γ\mathcal{N}(\delta_{v})=\gamma, for any place vv of FF, there is an element gvH~(Fvs)g_{v}\in\tilde{H}(F_{v}^{s}) such that gv1δvθ(gv)=tg^{-1}_{v}\delta_{v}\theta(g_{v})=t. We may even assume that g=(gv)H~(𝔸s)g=(g_{v})\in\tilde{H}(\mathbb{A}^{s}) by the following lemma.

Lemma 6.1.

Let GG be a (possibly disconnected) reductive group over a global field FF, and let tG(F)t\in G(F) be a semisimple element. Then outside of finitely many places vv of FF, for every δG(𝒪v)\delta\in G(\mathcal{O}_{v}) such that δ\delta is conjugate to tt under G(Fvs)G^{\circ}(F_{v}^{s}), there exists yG(𝒪vun)y\in G^{\circ}(\mathcal{O}^{\text{un}}_{v}) such that yty1=δyty^{-1}=\delta.

Here 𝒪v\mathcal{O}_{v} is the valuation ring of the completion FvF_{v} of FF at the place vv, and 𝒪vun\mathcal{O}^{\text{un}}_{v} is the valuation ring of the maximal unramified extension FvunF^{\text{un}}_{v} of FvF_{v}.

Proof.

We adapt the proof of Lemma 5 in [41]. Let XX denote the conjugacy class of tt under GG^{\circ}, and let i:XGi:X\hookrightarrow G denote the inclusion, it is a closed immersion since tt is semisimple. Let ff denote the morphism ggtg1g\mapsto gtg^{-1} from GG^{\circ} to XX. Then ff is smooth and surjective. There exists an ideal I𝒪FI\subset\mathcal{O}_{F}, which is the product of finitely many prime ideals, such that G,G,X,t,iG,G^{\circ},X,t,i and ff come from objects over 𝒪F[1I]\mathcal{O}_{F}[\frac{1}{I}]. We may assume that ff is smooth and surjective and ii is a closed immersion over 𝒪F[1I]\mathcal{O}_{F}[\frac{1}{I}] by replacing II with a suitable multiple.

Now we choose a place vv of FF outside of the finitely many places of II. By hypothesis δG(𝒪v)X(Fv)\delta\in G(\mathcal{O}_{v})\cap X(F_{v}), which is equal to X(𝒪v)X(\mathcal{O}_{v}), since ii is a closed immersion. The fiber YδY_{\delta} of f:GXf:G^{\circ}\to X over δX(𝒪v)\delta\in X(\mathcal{O}_{v}) is a smooth scheme of finite type over 𝒪v\mathcal{O}_{v}. The structural morphism YδSpec(𝒪v)Y_{\delta}\to\mathrm{Spec}(\mathcal{O}_{v}) is surjective since it is the composite of the following surjective morphisms:

Yδ{conjugacy class of δ under G}Spec(𝒪v)Y_{\delta}\longrightarrow\{\text{conjugacy class of }\delta\text{ under }G^{\circ}\}\longrightarrow\mathrm{Spec}(\mathcal{O}_{v})

hence the special fiber YδY_{\delta} is non-empty, and it has a point in some finite extension of the residue field of 𝒪v\mathcal{O}_{v}. Therefore by the smoothness of YδY_{\delta}, it has a point in the valuation ring of some finite unramified extension of FvF_{v}. Hence Yδ(𝒪vun)Y_{\delta}(\mathcal{O}^{\text{un}}_{v}) is non-empty, which means that there exists yG(𝒪vun)y\in G^{\circ}(\mathcal{O}^{\text{un}}_{v}) such that yγy1=δy\gamma y^{-1}=\delta. ∎

Remark 6.2.

Given the lemma above, we set G=H~θG=\tilde{H}\rtimes\langle\theta\rangle, hence G=H~1G^{\circ}=\tilde{H}\rtimes 1. We can regard t=(t,θ)G(F)t=(t,\theta)\in G(F) and similarly δG(𝔸)\delta\in G^{\circ}(\mathbb{A}). Outside of finitely many places, we have δvG(𝒪v)\delta_{v}\in G^{\circ}(\mathcal{O}_{v}). In this way, we can translate the fact that δv\delta_{v} and tt are θ\theta-conjugate under H~(Fvs)\tilde{H}(F^{s}_{v}) to that they are conjugate under G(Fvs)G^{\circ}(F^{s}_{v}), therefore we can apply the lemma to get gG(𝔸s)=H~(𝔸s)g\in G^{\circ}(\mathbb{A}^{s})=\tilde{H}(\mathbb{A}^{s}) such that

(6.1.1) g1δθ(g)=t.g^{-1}\delta\theta(g)=t.

Consider the map τtτ=g1τ(g)H~(𝔸s)\tau\mapsto t_{\tau}=g^{-1}\tau(g)\in\tilde{H}(\mathbb{A}^{s}) for τGal(Fs/F)\tau\in\mathrm{Gal}(F^{s}/F). We claim that tτt_{\tau} defines a 1-cocycle of Gal(Fs/F)\mathrm{Gal}(F^{s}/F) in T(𝔸s)T~(Fs)T(\mathbb{A}^{s})\tilde{T}(F^{s}). Indeed, apply τ\tau to (6.1.1) we get

(6.1.2) τ(g1)δθ(τ(g))=τ(t).\tau(g^{-1})\delta\theta(\tau(g))=\tau(t).

from (6.1.1) and (6.1.2) we get

(6.1.3) tττ(t)θ(tτ)1=tt_{\tau}\tau(t)\theta(t_{\tau})^{-1}=t

Apply the map NN on both sides, we get

tτN(τ(t))tτ1=Nt;t_{\tau}N(\tau(t))t_{\tau}^{-1}=Nt;

we have Nt=γNt=\gamma, and τ\tau commutes with NN since τ\tau commutes with θ\theta, hence we have tτγtτ1=γt_{\tau}\gamma t^{-1}_{\tau}=\gamma. Therefore we have tτT~(𝔸s)t_{\tau}\in\tilde{T}(\mathbb{A}^{s}). Then from (6.1.3) we know that tτθ(tτ)1=tτ(t)1T~(Fs)t_{\tau}\theta(t_{\tau})^{-1}=t\tau(t)^{-1}\in\tilde{T}(F^{s}), and we know that u=tτ(t1)u=t\tau(t^{-1}) satisfies Nu=1Nu=1. Since θ\theta acts on T~(Fs)=T(Fs)××T(Fs)\tilde{T}(F^{s})=T(F^{s})\times\dots\times T(F^{s}) by cyclic permutation, this implies that u=tτθ(tτ)1=tτ(t)1=vθ(v)1u=t_{\tau}\theta(t_{\tau})^{-1}=t\tau(t)^{-1}=v\theta(v)^{-1} for some vT~(Fs)v\in\tilde{T}(F^{s}). Then tτv1t_{\tau}v^{-1} is fixed by θ\theta, in other words, it belongs to T(𝔸s)T(\mathbb{A}^{s}). This shows that tτT(𝔸s)T~(Fs)t_{\tau}\in T(\mathbb{A}^{s})\tilde{T}(F^{s}). It is a 1-cocycle since by definition it is a coboundary in H~(𝔸s)\tilde{H}(\mathbb{A}^{s}).

Definition 6.3.

Let tτ:=g1τ(g)t_{\tau}:=g^{-1}\tau(g) for τGal(Fs/F)\tau\in\mathrm{Gal}(F^{s}/F). We take xτx_{\tau} to be the image of tτt_{\tau} in T(𝔸s)T~(Fs)/T~(Fs)=T(𝔸s)/T(Fs)T(\mathbb{A}^{s})\tilde{T}(F^{s})/\tilde{T}(F^{s})=T(\mathbb{A}^{s})/T(F^{s}), and define obs(δ)\rm{obs}(\delta) to be the class of (xτ)(x_{\tau}) in H1(F,T(𝔸s)/T(Fs))H^{1}(F,T(\mathbb{A}^{s})/T(F^{s})). This definition does not depend on the choice of gg or tt.

We have the following important property of obs(δ)\text{obs}(\delta):

Lemma 6.4.

obs(δ)H1(F,T(𝔸s)/T(Fs))\mathrm{obs}(\delta)\in H^{1}(F,T(\mathbb{A}^{s})/T(F^{s})) is trivial if and only if δ\delta is θ\theta-conjugate under H~(𝔸)\tilde{H}(\mathbb{A}) to an element of H~(F)\tilde{H}(F).

Proof.

The proof is the same as that of Lemma 6.2 in [10]. ∎

6.2. Pre-Stabilization

Now we assume that TT is an FF-torus of HH of the form T=HγT=H_{\gamma} for a strongly regular semisimple element γH(F)\gamma\in H(F) (recall that γ\gamma is strongly regular means that T=HγT=H_{\gamma} is a maximal torus, in particular, connected). We set D=H/HderD=H/H_{\text{der}} and D~=H~/H~der\tilde{D}=\tilde{H}/\tilde{H}_{\text{der}}, We have the following commutative diagram

T{\lx@inpgf@ignorespaces T}T~{\lx@inpgf@ignorespaces\tilde{T}}D{\lx@inpgf@ignorespaces D}D~{\lx@inpgf@ignorespaces\tilde{D}}

Dually, it becomes

D~^{\lx@inpgf@ignorespaces\hat{\tilde{D}}}T~^{\lx@inpgf@ignorespaces\hat{\tilde{T}}}D^{\lx@inpgf@ignorespaces\hat{D}}T^{\lx@inpgf@ignorespaces\hat{T}}

Those maps are all Γ\Gamma-equivariant.

We define the finite abelian groups

(6.2.1) A(T/F)\displaystyle A(T/F) =π0(T^Γ)/Imπ0(D~^Γ),\displaystyle=\pi_{0}(\hat{T}^{\Gamma})/\text{Im}\,\pi_{0}(\hat{\tilde{D}}^{\Gamma}),
A(T/Fv1)\displaystyle A(T/F_{v_{1}}) =π0(T^Γ1)/Imπ0(D~^Γ1).\displaystyle=\pi_{0}(\hat{T}^{\Gamma_{1}})/\text{Im}\,\pi_{0}(\hat{\tilde{D}}^{\Gamma_{1}}).

Where Γ1=Gal(Fv1s/Fv1)\Gamma_{1}=\mathrm{Gal}(F^{s}_{v_{1}}/F_{v_{1}}) is the decomposition group at the place v1v_{1} of FF.

The finite Abelian groups π0(T^Γ)\pi_{0}(\hat{T}^{\Gamma}) and H1(F,T(𝔸s)/T(Fs))H^{1}(F,T(\mathbb{A}^{s})/T(F^{s})) are canonically dual by [32]. Let <,><,> be the pairing between them with value in ×\mathbb{C}^{\times}. We claim that obs(δ)\text{obs}(\delta) has trivial image under the composition

H1(F,T(𝔸s)/T(Fs))π0(T^Γ)π0(D~^Γ)H^{1}(F,T(\mathbb{A}^{s})/T(F^{s}))\xrightarrow{\sim}\pi_{0}(\hat{T}^{\Gamma})^{*}\to\pi_{0}(\hat{\tilde{D}}^{\Gamma})^{*}

Indeed, since π0(D~^Γ)\pi_{0}(\hat{\tilde{D}}^{\Gamma})^{*} is canonically dual to H1(F,D~(𝔸s)/D~(Fs))H^{1}(F,\tilde{D}(\mathbb{A}^{s})/\tilde{D}(F^{s})), so we only need to find the image of obs(δ)\text{obs}(\delta) under the map

H1(F,T(𝔸s)/T(Fs))H1(F,D~(𝔸s)/D~(Fs)),H^{1}(F,T(\mathbb{A}^{s})/T(F^{s}))\to H^{1}(F,\tilde{D}(\mathbb{A}^{s})/\tilde{D}(F^{s})),

since obs(δ)\text{obs}(\delta) was constructed to be the class of tτ=g1τ(g)t_{\tau}=g^{-1}\tau(g) for some gH~(𝔸s)g\in\tilde{H}(\mathbb{A}^{s}), it splits when we project tτt_{\tau} to D~(𝔸s)\tilde{D}(\mathbb{A}^{s}). Hence for κA(T/F)\kappa\in A(T/F), we can further define the pairing obs(δ),κ\langle\text{obs}(\delta),\kappa\rangle\in\mathbb{C}. We have

obs(δ)=1obs(δ),κ=1 for all κA(T/F).\text{obs}(\delta)=1\Leftrightarrow\langle\text{obs}(\delta),\kappa\rangle=1\text{ for all }\kappa\in A(T/F).

We now begin the stabilization of the right hand side of the trace formula (5.2.1)

(6.2.2) δτ(Hδθ)TOδθH(𝔸E)(ϕ)\sum_{\delta}\tau(H_{\delta\theta})TO^{H(\mathbb{A}_{E})}_{\delta\theta}(\phi)

where we recall that the sum is over δH(E)\delta\in H(E) up to θ\theta-conjugacy under H(E)H(E) with NδN\delta regular elliptic. We also recall that ϕCc(H(𝔸E),λ1)\phi\in C^{\infty}_{c}(H(\mathbb{A}_{E}),\lambda^{-1}).

The global twisted orbital integral TOδθH(𝔸E)TO^{H(\mathbb{A}_{E})}_{\delta\theta} of ϕ\phi only depends on the H(𝔸E)H(\mathbb{A}_{E})-θ\theta-conjugacy class of δ\delta. We have the following lemma which allows us to regroup the elements in the summation:

Lemma 6.5.

The number of the terms in the sum that are indexed by the H(𝔸E)H(\mathbb{A}_{E})-θ\theta-conjugates of δ\delta is given by

|ker(ker1(F,Hδθ)ker1(F,H~))|=|ker1(F,Hδθ)||\ker(\ker^{1}(F,H_{\delta\theta})\to\ker^{1}(F,\tilde{H}))|=|\ker^{1}(F,H_{\delta\theta})|

where we have used the Hasse principle for H~\tilde{H}.

Proof.

We just need to look at the following diagram:

H1(F,Hδθ){\lx@inpgf@ignorespaces H^{1}(F,H_{\delta\theta})}vH1(Fv,Hδθ){\lx@inpgf@ignorespaces\prod_{v}H^{1}(F_{v},H_{\delta\theta})}H1(F,H~){\lx@inpgf@ignorespaces H^{1}(F,\tilde{H})}vH1(Fv,H~){\lx@inpgf@ignorespaces\prod_{v}H^{1}(F_{v},\tilde{H})}f\scriptstyle{\lx@inpgf@ignorespaces f}g\scriptstyle{\lx@inpgf@ignorespaces g}g\scriptstyle{\lx@inpgf@ignorespaces g^{\prime}}f\scriptstyle{\lx@inpgf@ignorespaces f^{\prime}}

Assume δ\delta^{\prime} is θ\theta-conjugate to δ\delta under H(𝔸E)H(\mathbb{A}_{E}) but not under H(E)H(E), then they are θ\theta-conjugate under H(Es)H(E^{s}) by Lemma 6.6, therefore corresponds to a cocycle τker(g)\tau\in\ker(g), which image f(τ)f(\tau) in vH1(Fv,Hδθ)\prod_{v}H^{1}(F_{v},H_{\delta\theta}) is trivial by assumption, that is to say, τker(ker1(F,Hδθ)ker1(F,H~))\tau\in\ker(\ker^{1}(F,H_{\delta\theta})\to\ker^{1}(F,\tilde{H})). Conversely, if τker(H1(F,Hδθ)H1(F,H~))\tau\in\ker(H^{1}(F,H_{\delta\theta})\to H^{1}(F,\tilde{H})), then we can associated a δH(E)\delta^{\prime}\in H(E) that is stably θ\theta-conjugate to δ\delta. The condition f(τ)=0f(\tau)=0 guarantees that δ\delta^{\prime} and δ\delta are θ\theta-conjugate under H(𝔸E)H(\mathbb{A}_{E}). ∎

Lemma 6.6.

Let KK be a global field and HH be a connected reductive group over KK. Let θ\theta be an KK-linear automorphism of HH. Let a,bH(K)a,b\in H(K) such that they are strongly θ\theta-regular semisimple and they are θ\theta-conjugate under H(𝔸K)H(\mathbb{A}_{K}), where 𝔸K\mathbb{A}_{K} is the ring of adeles of KK, then they are θ\theta-conjugated under H(Ks)H(K^{s}), where KsK^{s} is a fixed separable closure of KK.

Proof.

Indeed, the conditions imply that the algebraic variety X:={hH:h1aθ(h)=b}X:=\{h\in H:h^{-1}a\theta(h)=b\} has a point in KvsK^{s}_{v}, where vv is a place of KK and KvsK^{s}_{v} is a separable closure of the completion KvK_{v}. Since XX is defined by algebraic equations over KK as a,ba,b are rational over KK, this implies that X(K¯)X(\bar{K})\neq\emptyset, where K¯\bar{K} is an algebraic closure containing KsK^{s}. Since XX is isomorphic to HaθH_{a\theta} as schemes and the latter is geometrically reduced, since HaθH_{a\theta} is a connected torus, we have X(Ks)X(K^{s})\neq\emptyset, as desired. ∎

Therefore we can write (6.2.2) as

(6.2.3) δτ(Hδθ)|ker1(F,Hδθ)|TOδθH(𝔸E)(ϕ)\sum_{\delta}\tau(H_{\delta\theta})|\ker^{1}(F,H_{\delta\theta})|\,TO^{H(\mathbb{A}_{E})}_{\delta\theta}(\phi)

where the sum is over δH(E)\delta\in H(E) up to θ\theta-conjugacy under H(𝔸E)H(\mathbb{A}_{E}) with NδN\delta strongly elliptic regular.

Now we consider a strongly regular elliptic element γH(F)\gamma\in H(F) up to stable conjugacy, in other words, conjugacy under H(Fs)H(F^{s}) since γ\gamma is strongly regular. Assume δH(𝔸E)\delta\in H(\mathbb{A}_{E}) is such that its norm 𝒩δ\mathcal{N}\delta is equal to the stable class of γ\gamma at every place. The value of

1|A(T/F)|κA(T/F)obs(δ),κ\frac{1}{|A(T/F)|}\sum_{\kappa\in A(T/F)}\langle\text{obs}(\delta),\kappa\rangle

is 11 when δ\delta is θ\theta-conjugate to an element of H(E)H(E) under H(𝔸E)H(\mathbb{A}_{E}), by Lemma 6.4, and 00 otherwise since A(T/F)A(T/F) is a finite abelian group. Use this, we can write (6.2.3) as

(6.2.4) γH(F) strongly ell. reg.up to H(Fs)conjτ(T)|ker1(F,T)|δH(𝔸E)𝒩δ=γup to H(𝔸E)θconjugacy[1|A(T/F)|κA(T/F)obs(δ),κ]TOδθH(𝔸E)(ϕ)\begin{split}\sum_{\begin{subarray}{c}\gamma\in H(F)\text{ strongly ell. reg.}\\ \text{up to }H(F^{s})-\text{conj}\end{subarray}}&\tau(T)|\ker^{1}(F,T)|\\ &\sum_{\begin{subarray}{c}\delta\in H(\mathbb{A}_{E})\\ \mathcal{N}\delta=\gamma\\ \text{up to }H(\mathbb{A}_{E})-\theta-\text{conjugacy}\end{subarray}}[\frac{1}{|A(T/F)|}\sum_{\kappa\in A(T/F)}\langle\text{obs}(\delta),\kappa\rangle]TO^{H(\mathbb{A}_{E})}_{\delta\theta}(\phi)\end{split}

The equation 𝒩δ=γ\mathcal{N}\delta=\gamma holds for every place vv of EE. And we write T=HγT=H_{\gamma} for the centralizer for γ\gamma, which is isomorphic to HδθH_{\delta\theta} if δ\delta is a global element of norm γ\gamma.

In order to swap the order of the outer summations, we claim that the triple sum has only finitely many nonzero terms on any compact subset.

Lemma 6.7.

Fix a compact set CC of H(𝔸E)H(\mathbb{A}_{E}), then there are only finitely many θ\theta-conjugacy classes δ\delta under H(𝔸E)H(\mathbb{A}_{E}) that meet CC and such that 𝒩δ\mathcal{N}\delta is the class of a regular semisimple element of H(F)H(F).

Proof.

Following the same proof as in [35], we can reduce to case that NδN\delta is stably conjugate to a fixed regular semisimple element γ\gamma of H(F)H(F). We can find δ0H(E)\delta_{0}\in H(E) such that Nδ0=γN\delta_{0}=\gamma. Hence δ0\delta_{0} and δ\delta are stably θ\theta-conjugate. We assume that CC is contained in H(𝒪𝔸ES)×H(vSEv)H(\mathcal{O}_{\mathbb{A}^{S}_{E}})\times H(\prod_{v\in S}E_{v}), where SS is a finite set of fixed places of EE. We enlarge SS to apply Lemma 6.1. Now for any δC\delta\in C such that δ0,v\delta_{0,v} is stably θ\theta-conjugate to δv\delta_{v} for any place vSv\notin S, we view δ\delta and δ0\delta_{0} as (δ,θ)(\delta,\theta) and (δ0,θ)(\delta_{0},\theta) in the disconnected group HθH\ltimes\langle\theta\rangle, respectively. Hence (δ,θ)(\delta,\theta) is conjugate to (δ0,θ)(\delta_{0},\theta) under H(Evs)=(Hθ)(Evs)H(E_{v}^{s})=(H\ltimes\langle\theta\rangle)^{\circ}(E^{s}_{v}) in this sense. By Lemma 6.1, there exists gH(𝒪vun)g\in H(\mathcal{O}_{v}^{\text{un}}) such that δ\delta and δ0\delta_{0} are conjugate under gg. We claim that we can actually assume gH(Ov)g\in H(O_{v}).

Indeed, consider the cocycle τg:θg1θ(g)\tau_{g}:\theta\mapsto g^{-1}\theta(g), here we use θ\theta to denote the topological generator of Gal(Fun/F)\mathrm{Gal}(F^{\text{un}}/F). It is clear that τg\tau_{g} is a 1-cocycle in 𝒯(𝒪vun):=Hγ(𝒪vun)\mathcal{T}(\mathcal{O}_{v}^{\text{un}}):=H_{\gamma}(\mathcal{O}_{v}^{\text{un}}), by applying θ\theta on the equation g1δvg=δ0,vg^{-1}\delta_{v}g=\delta_{0,v}. Here we use the existence of lft Neron model 𝒯\mathcal{T} associated to T=HγT=H_{\gamma} over 𝒪vun\mathcal{O}_{v}^{\text{un}}. Hence τgH1(θ,𝒯(𝒪vun))\tau_{g}\in H^{1}(\langle\theta\rangle,\mathcal{T}(\mathcal{O}_{v}^{\text{un}})). It is trivial by (7.6.1) of [38], hence there exists t𝒯(𝒪vun)t\in\mathcal{T}(\mathcal{O}_{v}^{\text{un}}) such that g1θ(g)=t1θ(t)g^{-1}\theta(g)=t^{-1}\theta(t), in other words, gt1H(𝒪vun)H(Fv)=H(Ov)gt^{-1}\in H(\mathcal{O}^{\text{un}}_{v})\cap H(F_{v})=H(O_{v}). Replace gg by gt1gt^{-1}, the claim is proved.

Now for every θ\theta-conjugacy class δ\delta that meet CC and 𝒩δ=γ\mathcal{N}\delta=\gamma, we know for vSv\notin S, the θ\theta-conjugacy class of δv\delta_{v} contains δ0,v\delta_{0,v}, and for every place wSw\in S, there are only finitely many θ\theta-conjugacy classes inside a fixed stable θ\theta-conjugacy class. Therefore, there are only finitely many such θ\theta-conjugacy classes δ\delta satisfying those conditions when CH(𝔸E)C\subset H(\mathbb{A}_{E}). ∎

Therefore, we can reorder the sum in (6.2.4) as

(6.2.5) γτ(T)|ker1(F,T)||A(T,F)|κδobs(δ),κTOδθH(𝔸E)(ϕ).\sum_{\gamma}\tau(T)\frac{|\ker^{1}(F,T)|}{|A(T,F)|}\sum_{\kappa}\sum_{\delta}\langle\text{obs}(\delta),\kappa\rangle TO^{H(\mathbb{A}_{E})}_{\delta\theta}(\phi).

Where each index is summing over the same set as in (6.2.4).

6.3. Vanishing of Kappa Orbital Integrals

Consider the inner sum in (6.2.5)

(6.3.1) δobs(δ),κTOδθH(𝔸E)(ϕ)\sum_{\delta}\langle\text{obs}(\delta),\kappa\rangle TO^{H(\mathbb{A}_{E})}_{\delta\theta}(\phi)

where the summation is over H(𝔸E)H(\mathbb{A}_{E})-θ\theta-conjugacy classes of δH(𝔸E)\delta\in H(\mathbb{A}_{E}) such that 𝒩δ=γ\mathcal{N}\delta=\gamma locally everythere, for an elliptic strongly regular γH(F)\gamma\in H(F) up to conjugacy by H(Fs)H(F^{s}).

We assume that there is a θ\theta-elliptic, θ\theta-strongly regular δ0H(𝔸E)\delta^{0}\in H(\mathbb{A}_{E}) such that 𝒩δ0=γ\mathcal{N}\delta^{0}=\gamma holds. Otherwise, the sum in (6.3.1) would be empty. Therefore, the summation in (6.3.1) will be over the global θ\theta-conjugacy classes within the global stable θ\theta-conjugacy class of δ0\delta^{0}, by Proposition 2.16.

We know that the θ\theta-conjugacy classes within the stable θ\theta-conjugacy class of δv0\delta^{0}_{v}, the local component of δ0\delta^{0} at vv, are in bijection with

𝒟θ(Iv/Fv):=ker(H1(Fv,Iv)H1(Fv,H~)),\mathcal{D}_{\theta}(I_{v}/F_{v}):=\ker(H^{1}(F_{v},I_{v})\to H^{1}(F_{v},\tilde{H})),

where IvI_{v} is the θ\theta-centralizer of δv0\delta^{0}_{v} in H~Fv\tilde{H}_{F_{v}}. We notice that Iv=IvI_{v}=I^{\circ}_{v} by assumptions on δ0\delta^{0}.

The next goal is to write (6.3.1) as a product of local sums. If δ=(δv)\delta=(\delta_{v}) is in the (global) stable θ\theta-conjugacy class of δ0\delta_{0}, by above we can write (δv)=(xvδv0)(\delta_{v})=(x_{v}\cdot\delta^{0}_{v}) where x=(xv)v𝒟θ(Iv/Fv)x=(x_{v})\in\bigoplus_{v}\mathcal{D}_{\theta}(I_{v}/F_{v}). Let inv(δ,δ0)H1(F,T(𝔸s)/T(Fs))\text{inv}(\delta,\delta^{0})\in H^{1}(F,T(\mathbb{A}^{s})/T(F^{s})) be the image of (xv)(x_{v}) under the maps

v𝒟θ(Iv/Fv)vH1(Fv,T(Fv))H1(F,T(𝔸s)/T(Fs)),\bigoplus_{v}\mathcal{D}_{\theta}(I_{v}/F_{v})\to\bigoplus_{v}H^{1}(F_{v},T(F_{v}))\to H^{1}(F,T(\mathbb{A}^{s})/T(F^{s})),

where the first map is given by the canonical isomorphisms between IvI_{v} and T(Fv)T(F_{v}), where T=HγT=H_{\gamma}. From the definitions of obs(δ)\text{obs}(\delta) and inv(δ,δ0)\text{inv}(\delta,\delta^{0}), we see that

obs(δ)=inv(δ,δ0)obs(δ0).\text{obs}(\delta)=\text{inv}(\delta,\delta^{0})\text{obs}(\delta^{0}).

Therefore, assuming ϕ=vϕv\phi=\bigotimes_{v}\phi_{v} (over places of FF) is a pure tensor product element in Cc(H(𝔸E))Cc(H~(𝔸F))C^{\infty}_{c}(H(\mathbb{A}_{E}))\cong C^{\infty}_{c}(\tilde{H}(\mathbb{A}_{F})), therefore we can write (6.3.1), when the sum is nonempty, as

(6.3.2) obs(δ0),κv(xv𝒟θ(Iv/Fv)xv,κvTOxvδv0,θH(Ev)(ϕv))\langle\text{obs}(\delta^{0}),\kappa\rangle\,\prod_{v}(\sum_{x_{v}\in\mathcal{D}_{\theta}(I_{v}/F_{v})}\langle x_{v},\kappa_{v}\rangle TO^{H(E_{v})}_{x_{v}\cdot\delta^{0}_{v},\theta}(\phi_{v}))

which we write as

(6.3.3) obs(δ0),κvOδv0,θκv(ϕv)\langle\text{obs}(\delta^{0}),\kappa\rangle\,\prod_{v}O^{\kappa_{v}}_{\delta^{0}_{v},\theta}(\phi_{v})

where we denote the κv\kappa_{v}-twisted orbital integral,

Oδv0,θκv(ϕv):=xv𝒟θ(Iv/Fv)xv,κTOxvδv0,θH(Ev)(ϕv),O^{\kappa_{v}}_{\delta^{0}_{v},\theta}(\phi_{v}):=\sum_{x_{v}\in\mathcal{D}_{\theta}(I_{v}/F_{v})}\langle x_{v},\kappa\rangle TO^{H(E_{v})}_{x_{v}\cdot\delta^{0}_{v},\theta}(\phi_{v}),

and κv𝒟θ(Iv/Fv)\kappa_{v}\in\mathcal{D}_{\theta}(I_{v}/F_{v})^{*} is the local image of κ\kappa.

We have arrived at the vanishing results of this section:

Lemma 6.8.

Assume ϕ=vϕv\phi=\bigotimes_{v}\phi_{v} is a pure tensor product element in ϕCc(H(𝔸E),λ1)\phi\in C^{\infty}_{c}(H(\mathbb{A}_{E}),\lambda^{-1}) over places vv of FF, and at some place v1v_{1} of FF, the following two conditions hold:

  1. (1)

    TOδv1,θH(Ev)(ϕv1)=0TO^{H(E_{v})}_{\delta_{v_{1}},\theta}(\phi_{v_{1}})=0 for all elements δv1H~(Fv1)=H(EFv1)\delta_{v_{1}}\in\tilde{H}(F_{v_{1}})=H(E\,\otimes F_{v_{1}}) that are not θ\theta-elliptic, and for θ\theta-elliptic θ\theta-regular elements δv1\delta_{v_{1}}, the twisted orbital integral is constant on stable θ\theta-conjugacy classes of δv1\delta_{v_{1}}.

  2. (2)

    There exists a finite Galois extension LL of FF such that Lv1L_{v_{1}} is a field and LL splits D~\tilde{D}.

Then

(6.3.4) δobs(δ),κTOδθH(𝔸E)(ϕ)=0\sum_{\delta}\langle\mathrm{obs}(\delta),\kappa\rangle TO^{H(\mathbb{A}_{E})}_{\delta\theta}(\phi)=0

if κ\kappa is nontrivial in A(T/F)A(T/F).

Remark 6.9.

If ϕ\phi and HH indeed satisfy the conditions in the lemma, the sum (6.2.5) would reduce to its stable part:

(6.3.5) γτ(T)|ker1(F,T)||A(T,F)|δTOδθ(ϕ),\sum_{\gamma}\tau(T)\frac{|\ker^{1}(F,T)|}{|A(T,F)|}\sum_{\delta}TO_{\delta\theta}(\phi),

which means that the summation over κ\kappa only has κ=1\kappa=1 left.

Proof.

As in [10], Lemma 6.5, it boils down to the following lemma. ∎

Lemma 6.10.

Suppose there exists a finite Galois extension LL of FF such that Lv1L_{v_{1}} is a field and LL splits D~.\tilde{D}. Suppose TT is a maximal FF-torus in HH which is elliptic at v1v_{1}, then the canonical map

A(T/F)A(T/Fv1)A(T/F)\to A(T/F_{v_{1}})

is injective.

Proof.

As in the proof of Lemma 8.4.1 of [18] and Lemma 6.5 in [10], we simply notice that D~^Γ=D~^Γ1=D~^Γ\hat{\tilde{D}}^{\Gamma}=\hat{\tilde{D}}^{\Gamma_{1}}=\hat{\tilde{D}}^{\Gamma^{\prime}}, where Γ=Gal(Lv1/Fv1)\Gamma^{\prime}=\mathrm{Gal}(L_{v_{1}}/F_{v_{1}}). ∎

Functions with properties in Lemma 6.8(a) are called generalized Kottwitz functions (see [44] 3.9 and [18] 8.2). We will discuss them further when we move to the global setup in 11.2.

6.4. End of Stabilization

From now on, we assume that ϕ\phi satisfies the conditions of Lemma 6.8. Following [10], we see that the elliptic regular term of the twisted trace formula (6.3.5) is equal to

(6.4.1) c(H)γH(F) strongly ell. reg.up to H(Fs)conjτ(T)|ker1(F,T)||π0(D^Γ)||π0(T^Γ)|δH(𝔸E)𝒩δ=γup to H(𝔸E)θconjugacyTOδθ(ϕ),c(H)\sum_{\begin{subarray}{c}\gamma\in H(F)\text{ strongly ell. reg.}\\ \text{up to }H(F^{s})-\text{conj}\end{subarray}}\tau(T)|\ker^{1}(F,T)|\frac{|\pi_{0}(\hat{D}^{\Gamma})|}{|\pi_{0}(\hat{T}^{\Gamma})|}\sum_{\begin{subarray}{c}\delta\in H(\mathbb{A}_{E})\\ \mathcal{N}\delta=\gamma\\ \text{up to }H(\mathbb{A}_{E})-\theta-\text{conjugacy}\end{subarray}}TO_{\delta\theta}(\phi),

with

(6.4.2) c(H)=|Imπ0(D~^Γ)||π0(D^Γ)|.c(H)=\frac{|\text{Im}\,\pi_{0}(\hat{\tilde{D}}^{\Gamma})|}{|\pi_{0}(\hat{D}^{\Gamma})|}.

We assume HH satisfies the Hasse principle for H1H^{1}, and that f=vfvCc(H(𝔸),λ1)f=\bigotimes_{v}f_{v}\in C^{\infty}_{c}(H(\mathbb{A}),\lambda^{-1}) satisfies the analogs of conditions (a) and (b) in Lemma 6.8. In other words, we regard E=FE=F and θ=id\theta=\text{id}. Then the elliptic strongly regular part of the trace formula for ff, by the same stabilization process, reduces to

(6.4.3) γH(F) strongly ell. reg.up to H(Fs)conjτ(T)|ker1(F,T)||π0(D^Γ)||π0(T^Γ)|γH(𝔸)γ stably conjugate to γup to H(𝔸)conjugacyOγ(f).\sum_{\begin{subarray}{c}\gamma\in H(F)\text{ strongly ell. reg.}\\ \text{up to }H(F^{s})-\text{conj}\end{subarray}}\tau(T)|\ker^{1}(F,T)|\frac{|\pi_{0}(\hat{D}^{\Gamma})|}{|\pi_{0}(\hat{T}^{\Gamma})|}\sum_{\begin{subarray}{c}\gamma^{\prime}\in H(\mathbb{A})\\ \gamma^{\prime}\text{ stably conjugate to }\gamma\\ \text{up to }H(\mathbb{A})-\text{conjugacy}\end{subarray}}O_{\gamma^{\prime}}(f).

Since the last sums in (6.4.1) and (6.4.3) can be expressed as products of local orbital integrals over places vv of FF, as we discussed before, we see that if ϕ\phi and ff have matching stable orbital integrals at every place of FF, the two expressions (6.4.1) and (6.4.3) agree up to the factor c(H)c(H), that is:

Proposition 6.11.

Let ϕ=vϕvCc(H(𝔸E),λ1)\phi=\bigotimes_{v}\phi_{v}\in C^{\infty}_{c}(H(\mathbb{A}_{E}),\lambda^{-1}) and f=vfvCc(H(𝔸),λ1)f=\bigotimes_{v}f_{v}\in C^{\infty}_{c}(H(\mathbb{A}),\lambda^{-1}) be functions satisfying the conditions in 5.2 (1)(2)(3) and Lemma 6.8 (a). Assume γG(F)\gamma\in G(F) and the image γ¯H(F)=Gad(F)\bar{\gamma}\in H(F)=G_{\rm ad}(F) are strongly elliptic regular in the respective groups, δG(𝔸E)\delta\in G(\mathbb{A}_{E}) such that 𝒩δ=γ\mathcal{N}\delta=\gamma locally everywhere (therefore we also have 𝒩δ¯=γ¯\mathcal{N}\bar{\delta}=\bar{\gamma}, and δv\delta_{v} (resp. δ¯v\bar{\delta}_{v}) is θ\theta-strongly regular θ\theta-elliptic in G(Ev)G(E_{v}) (resp. H(Ev)H(E_{v}))). If we have for every place vv of FF

(6.4.4) SOδvθG(Ev)=SOγvG(Ev),SO^{G(E_{v})}_{\delta_{v}\theta}=SO^{G(E_{v})}_{\gamma_{v}},

for every such δG(𝔸E)\delta\in G(\mathbb{A}_{E}) and γG(F)\gamma\in G(F) then there exists a constant c>0c>0 such that

(6.4.5) tr(Rcusp(ϕ)Iθ)=ctr(rcusp(f)).\mathrm{tr}(R_{\mathrm{cusp}}(\phi)\circ I_{\theta})=c\,\mathrm{t}r(r_{\mathrm{cusp}}(f)).
Proof.

By the stabilization process in this section, we know that

tr(Rcusp(ϕ)Iθ)=(6.4.1)tr(rcusp(f))=(6.4.3).\begin{split}\mathrm{tr}(R_{\text{cusp}}(\phi)\circ I_{\theta})=(\ref{6.4.1})\\ \mathrm{tr}(r_{\text{cusp}}(f))=(\ref{6.4.3}).\end{split}

And we know that (6.4.1)=c(H)(6.4.3)(\ref{6.4.1})=c(H)\cdot(\ref{6.4.3}) provided

SOδ¯vθH(Ev)=SOγ¯vH(Ev)SO^{H(E_{v})}_{\bar{\delta}_{v}\theta}=SO^{H(E_{v})}_{\bar{\gamma}_{v}}

for every place vv of FF. By Lemma 5.16, this is equivalent to (6.4.4), as desired. ∎

7. Proof In the Strongly Regular Elliptic Case

7.1. Local Data

We first give the definition of the local data, which is the necessary bridge between spectral side geometric side of the theory. We assume GG is any unramified reductive group defined over local field FF. Let E/FE/F be an unramified extension of degree rr, denote θ\theta to be a generator of Gal(E/F)\mathrm{Gal}(E/F) as usual. Let Gr:=G(E)G_{r}:=G(E).

Let Irrχ,λ(G)\text{Irr}_{\chi,\lambda}(G) (resp. Irrχr,λrθ(Gr)\text{Irr}^{\theta}_{\chi_{r},\lambda_{r}}(G_{r})) denote the set of irreducible (resp. irreducible θ\theta-stable) admissible representations in χ(G)\mathfrak{R}_{\chi}(G) (resp. χr(Gr)\mathfrak{R}_{\chi_{r}}(G_{r})) that transformed by λ\lambda (resp. λr\lambda_{r}) under the center action. We define (Gr,ρr,λr1)\mathcal{H}(G_{r},\rho_{r},\lambda^{-1}_{r}) to the algebra of compactly supported functions on Gr/Z(Gr)G_{r}/Z(G_{r}) transformed by ρr\rho_{r} (resp. λ1\lambda^{-1}) under the subgroups IrI_{r} (resp. Z(Gr)Z(G_{r})), and similarly for (G,ρ,λ1)\mathcal{H}(G,\rho,\lambda^{-1}).

We define the local data adapted to Irrχ,λ(G)\text{Irr}_{\chi,\lambda}(G) to consist of data (a), (b) and (c), subject to conditions (1) and (2) below:

  1. (1)

    An index set λ\mathcal{I}_{\lambda}, possibly infinite;

  2. (2)

    A collection of complex numbers ai(π)a_{i}(\pi) for iλi\in\mathcal{I}_{\lambda} and πIrrχ,λ(G)\pi\in\text{Irr}_{\chi,\lambda}(G);

  3. (3)

    A collection of complex numbers bi(Π)b_{i}(\Pi) for iλi\in\mathcal{I}_{\lambda} and ΠIrrχr,λrθ(Gr)\Pi\in\text{Irr}^{\theta}_{\chi_{r},\lambda_{r}}(G_{r}).

  1. (1)

    For an fixed ii, the constants ai(π)a_{i}(\pi) and bi(Π)b_{i}(\Pi) are zero for all but finitely many π\pi and Π\Pi.

  2. (2)

    For ϕ(Gr,ρr,λr1)\phi\in\mathcal{H}(G_{r},\rho_{r},\lambda^{-1}_{r}) and f(G,ρ,λ1)f\in\mathcal{H}(G,\rho,\lambda^{-1}), the following statements are equivalent:

    1. (a)

      For all iλi\in\mathcal{I}_{\lambda}, we have πai(π)trπ,f=Πbi(Π)trΠIθ,ϕ\sum_{\pi}a_{i}(\pi)\langle\text{tr}\,\pi,f\rangle=\sum_{\Pi}b_{i}(\Pi)\langle\text{tr}\,\Pi I_{\theta},\phi\rangle;

    2. (b)

      For all strongly regular elliptic semisimple norms γ=𝒩(δ)\gamma=\mathcal{N}(\delta), where γG\gamma\in G and δGr\delta\in G_{r}, we have

      SOγ(f)=SOδθ(ϕ).SO_{\gamma}(f)=SO_{\delta\theta}(\phi).
Remark 7.1.

Since GG might not have a compact center and the functions we consider here are only compactly supported mod centers, the trace trπ,f\langle\mathrm{tr}\,\pi,f\rangle (resp. trΠIθ,ϕ\langle\mathrm{tr}\,\Pi I_{\theta},\phi\rangle) should be understood to be over G/ZG/Z (resp. Gr/ZrG_{r}/Z_{r}) instead of over GG (resp. GrG_{r}), as the action (5.1.2) is over G/ZG/Z (resp. Gr/ZrG_{r}/Z_{r}).

7.2. Global Setup

From now on, we embed the local situation into a suitable global setup, in order to apply the stabilizations of (twisted) simple trace formula to prove the existence of the local data.

We assume Gder=GscG_{\text{der}}=G_{\text{sc}}. We may assume that GG is split over an unramified extension K/FK/F such that EKE\subset K. We choose a degree [K:F][K:F] cyclic extension of global function fields K¯/F¯\underline{K}/\underline{F} and a finite place v0v_{0} of F¯\underline{F} such that K¯v0\underline{K}_{v_{0}} is a field and K¯v0/F¯v0K/F\underline{K}_{v_{0}}/\underline{F}_{v_{0}}\cong K/F. Then there is a degree r=[E:F]r=[E:F] cyclic extension E¯/F¯\underline{E}/\underline{F} with E¯K¯\underline{E}\subset\underline{K} and E¯v0/F¯v0E/F\underline{E}_{v_{0}}/\underline{F}_{v_{0}}\cong E/F.

The Tchebotarev density theorem is still valid in positive characteristics (for example, see [29]), therefore we can find an inert place v1v_{1} of F¯\underline{F}, v1v0v_{1}\neq v_{0} with Gal(K¯v1/F¯v1)=Gal(K/F)\mathrm{Gal}(\underline{K}_{v_{1}}/\underline{F}_{v_{1}})=\mathrm{Gal}(K/F). In addition, we fix two more auxiliary finite places v2v_{2} and v3v_{3} of F¯\underline{F} where E¯/F¯\underline{E}/\underline{F} splits completely at these places. We can assume that v0{v1,v2,v3}v_{0}\notin\{v_{1},v_{2},v_{3}\}.

There is a quasi-split group G¯\underline{G} over F¯\underline{F} with the property that G¯×F¯F¯v0G\underline{G}\times_{\underline{F}}\underline{F}_{v_{0}}\cong G. We set G¯~=ResE¯/F¯G¯E¯\tilde{\underline{G}}=\mathrm{Res}_{\underline{E}/\underline{F}}\underline{G}_{\underline{E}}. By the reduction steps, we can assume that Z(G¯)Z(\underline{G}) is an induced torus over FF, and denote H¯=G¯/Z(G¯)\underline{H}=\underline{G}/Z(\underline{G}). Let θ\theta denote the F¯\underline{F}-linear automorphism of G¯~\tilde{\underline{G}} from θ=Gal(E/F)Gal(E¯/F¯)\theta=\mathrm{Gal}(E/F)\cong\mathrm{Gal}(\underline{E}/\underline{F}).

We may assume that the groups G¯\underline{G} and G¯~\tilde{\underline{G}} have simply connected derived subgroups and split over K¯\underline{K}. In order to apply the stabilization results in §6, they have to satisfy the Hasse principle for H1H^{1} on H¯\underline{H} and H¯~\tilde{\underline{H}}, namely ker1(F¯,H¯)=ker1(F¯,H¯~)=1\ker^{1}(\underline{F},\underline{H})=\ker^{1}(\underline{F},\tilde{\underline{H}})=1. Since viv_{i} splits completely for i=2,3i=2,3, we have identifications

G¯(E¯vi)=G¯(F¯vi)××G¯(F¯vi)\underline{G}(\underline{E}_{v_{i}})=\underline{G}(\underline{F}_{v_{i}})\times\dots\times\underline{G}(\underline{F}_{v_{i}})

with rr factors, and Gal(E¯vi/F¯vi)\mathrm{Gal}(\underline{E}_{v_{i}}/\underline{F}_{v_{i}}) acts by cyclic permutations. Same decompositions and permutations hold for H¯(E¯vi)\underline{H}(\underline{E}_{v_{i}}).

We write ϕ¯=ϕv0ϕv0=vϕv\underline{\phi}=\phi^{v_{0}}\otimes\phi_{v_{0}}=\otimes_{v}\phi_{v} for a pure tensor element of Cc(H¯(𝔸E¯),λ1)C^{\infty}_{c}(\underline{H}(\mathbb{A}_{\underline{E}}),\lambda^{-1}) for a global unitary character λ:Z¯(𝔸E¯)/Z¯(E¯)×\lambda:\underline{Z}(\mathbb{A}_{\underline{E}})/\underline{Z}(\underline{E})\to\mathbb{C}^{\times} over places of F¯\underline{F} and similarly f¯=fv0fv0=vfv\underline{f}=f^{v_{0}}\otimes f_{v_{0}}=\otimes_{v}f_{v}. We write ϕ\phi for ϕv0\phi_{v_{0}} and ff for fv0f_{v_{0}}.

We will always use the symbol S3S_{3} to denote a finite set of places of F¯\underline{F} such that v3S3v_{3}\in S_{3} and v1,v2S3v_{1},v_{2}\notin S_{3}. Finally, we consider triples (ϕv0,fv0,S3)(\phi^{v_{0}},f^{v_{0}},S_{3}) satisfying the following conditions.

  1. (1)

    At any place vS3{v1,v2}v\notin S_{3}\cup\{v_{1},v_{2}\}, the group G¯×F¯F¯v\underline{G}\times_{\underline{F}}\underline{F}_{v} and the extension E¯v/F¯v\underline{E}_{v}/\underline{F}_{v} are unramified.

  2. (2)

    The function fv1f_{v_{1}} (resp. ϕv1\phi_{v_{1}}) is (up to a scalar) a pullback of generalized Kottwitz function on H¯(F¯v1)\underline{H}(\underline{F}_{v_{1}}) (resp., H¯~(F¯v1)\tilde{\underline{H}}(\underline{F}_{v_{1}})) satisfying the conditions in Lemma 6.8 (a). In particular, λv1=triv\lambda_{v_{1}}=\text{triv}. Moreover, we may assume they are associated, as in §8.2 of [18]. We notice that this construction requires that E/FE/F is inert at v1v_{1}.

  3. (3)

    The function fv2f^{\prime}_{v_{2}} is a coefficient of a supercuspidal representation, ϕv2=fv2fv2\phi_{v_{2}}=f^{\prime}_{v_{2}}\otimes\dots\otimes f^{\prime}_{v_{2}} and fv2=fv2fv2f_{v_{2}}=f^{\prime}_{v_{2}}\ast\dots\ast f^{\prime}_{v_{2}}. Thus (ϕv2,fv2)(\phi_{v_{2}},f_{v_{2}}) are associated and have nonvanishing (twisted) orbital integrals at (θ)(\theta)-elliptic strongly (θ)(\theta)-regular elements which are close to the identity. Notice that these functions are only compactly supported modulo centers.

  4. (4)

    For any vS3v\in S_{3}, fvf_{v} (resp., ϕv\phi_{v}) is supported on the set of strongly regular elements (resp., elements with strongly regular norms), and (ϕv,fv)(\phi_{v},f_{v}) are associated. Moreover, the function fv3f_{v_{3}} (resp., ϕv3\phi_{v_{3}}) is supported on the set of elliptic elements with strongly regular elliptic images in G(F¯v3)G^{*}(\underline{F}_{v_{3}}) (resp., elements with elliptic norms).

  5. (5)

    For any other place vS3{v0,v1,v2}v\notin S_{3}\cup\{v_{0},v_{1},v_{2}\}, the function fvf^{\prime}_{v} (resp., ϕv\phi^{\prime}_{v}) is the unit element of the spherical Hecke algebra of H¯(F¯v)\underline{H}(\underline{F}_{v}) (resp., H¯(E¯v)\underline{H}(\underline{E}_{v})). Then (ϕv,fv)(\phi^{\prime}_{v},f^{\prime}_{v}) are associated by [34]. We then form the function ϕv\phi_{v} (resp., fvf_{v}) to be the pullback of ϕv\phi^{\prime}_{v} (resp., fvf^{\prime}_{v}) with the trivial central action. Therefore (ϕv,fv)(\phi_{v},f_{v}) are associated by Lemma 5.16.

  6. (6)

    At every place vv of F¯\underline{F} where E¯/F¯\underline{E}/\underline{F} splits, we have ϕv=fvfv\phi_{v}=f^{\prime}_{v}\otimes\dots\otimes f^{\prime}_{v} and fv=fvfvf_{v}=f^{\prime}_{v}\ast\dots\ast f^{\prime}_{v} for an appropriate function fvf^{\prime}_{v} so that (ϕv,fv)(\phi_{v},f_{v}) are associated.

We note that by the above conditions, the functions fvf_{v} and ϕv\phi_{v} are assumed to be associated at every place vv0v\neq v_{0}.

7.3. Existence of the Local Data

We prove that local data adapted to Irrχ,λ(G)\text{Irr}_{\chi,\lambda}(G) in this subsection.

By abuse of notations, we use R(ϕ¯)R(\underline{\phi}) (resp. R(f¯)R(\underline{f})) to denote the action of ϕ¯\underline{\phi} (resp., f¯\underline{f}) on the cuspidal spectrum Lcusp2(H¯(E¯)\H¯(𝔸E¯),λ)L^{2}_{\text{cusp}}(\underline{H}(\underline{E})\backslash\underline{H}(\mathbb{A}_{\underline{E}}),\lambda) (resp., Lcusp2(H¯(F¯)\H¯(𝔸F¯),λ)L^{2}_{\text{cusp}}(\underline{H}(\underline{F})\backslash\underline{H}(\mathbb{A}_{\underline{F}}),\lambda)). Let IθI_{\theta} denote the intertwining operator on the same space given by Iθ(ψ)(x):=ψ(θ1(x))I_{\theta}(\psi)(x):=\psi(\theta^{-1}(x)) for ψLcusp2(H¯(E¯)\H¯(𝔸E¯),λ)\psi\in L^{2}_{\text{cusp}}(\underline{H}(\underline{E})\backslash\underline{H}(\mathbb{A}_{\underline{E}}),\lambda) and xH¯(𝔸E¯)x\in\underline{H}(\mathbb{A}_{\underline{E}}). The existence of local data comes from the following proposition. We say that fv0f_{v_{0}} and ϕv0\phi_{v_{0}} are associated at strongly regular elliptic norms if they are associated for every strongly regular elliptic semisimple norm in the adjoint group γ=𝒩δ\gamma=\mathcal{N}\delta in G¯(F¯v0)\underline{G}(\underline{F}_{v_{0}}) whose image γ¯\bar{\gamma} is also strongly regular elliptic semisimple in H¯(F¯v0)\underline{H}(\underline{F}_{v_{0}}).

Proposition 7.2.

There is a constant c0c\neq 0, depending only on (G¯,E¯/F¯)(\underline{G},\underline{E}/\underline{F}), with the following property: the functions fv0f_{v_{0}} and ϕv0\phi_{v_{0}} are associated at strongly regular norms if and only we have the equality of traces

(7.3.1) tr(R(ϕv0ϕv0)Iθ)=ctrR(fv0fv0),\mathrm{tr}(R(\phi^{v_{0}}\otimes\phi_{v_{0}})I_{\theta})=c\,\mathrm{tr}\,R(f^{v_{0}}\otimes f_{v_{0}}),

for every triple (ϕv0,fv0,S3)(\phi^{v_{0}},f^{v_{0}},S_{3}) satisfying conditions (a)-(f) in §7.2.

Proof.

For the ”if” part, at the place v0v_{0}, if we are given γ0=𝒩δ0\gamma_{0}=\mathcal{N}\delta_{0} for (resp. θ\theta-) strongly regular elliptic semisimple element γ0G¯(F¯v0)\gamma_{0}\in\underline{G}(\underline{F}_{v_{0}}) (resp. δ0G¯(E¯v0)\delta_{0}\in\underline{G}(\underline{E}_{v_{0}}) ), we choose an appropriate global element δG¯~(F¯)\delta\in\underline{\tilde{G}}(\underline{F}) such that:

  1. (1)

    δv0\delta_{v_{0}} is close to δ0\delta_{0} at v0v_{0} and close to 11 at v2v_{2};

  2. (2)

    δvi\delta_{v_{i}} is θ\theta-elliptic and strongly θ\theta-regular at i=1,2,3i=1,2,3.

Thus δ\delta itself is θ\theta-elliptic and strongly θ\theta-regular. Then we can choose the set S3S_{3} and the associated functions (fv0,ϕv0)(f^{v_{0}},\phi^{v_{0}}) such that, the geometric sides of (7.3.1), according to the stabilization process, take the stabilized form of equations (6.4.1) and (6.4.3), which involve only the term indexed by γ:=𝒩δ\gamma:=\mathcal{N}\delta. The second sums in those equations, which are the sum of adelic (twisted) orbital integrals can be written as a product over all places of local stable (twisted) orbital integrals, and at all places except v0v_{0}, these are nonzero (by choice) and matching. Then the identity (7.3.1) will force the matching at v0v_{0}, namely, SOδv0θH¯(E¯v0)(ϕv0)=SOγv0H¯(F¯v0)(fv0)SO^{\underline{H}(\underline{E}_{v_{0}})}_{\delta_{v_{0}}\theta}(\phi_{v_{0}})=SO^{\underline{H}(\underline{F}_{v_{0}})}_{\gamma_{v_{0}}}(f_{v_{0}}). By Lemma 5.16, we then have SOδv0θG¯(E¯v0)(ϕv0)=SOγv0G¯(F¯v0)(fv0)SO^{\underline{G}(\underline{E}_{v_{0}})}_{\delta_{v_{0}}\theta}(\phi_{v_{0}})=SO^{\underline{G}(\underline{F}_{v_{0}})}_{\gamma_{v_{0}}}(f_{v_{0}}). A continuity argument then forces the desired identity SOδ0θG¯(E¯v0)(ϕv0)=SOγ0G¯(F¯v0)(fv0)SO^{\underline{G}(\underline{E}_{v_{0}})}_{\delta_{0}\theta}(\phi_{v_{0}})=SO^{\underline{G}(\underline{F}_{v_{0}})}_{\gamma_{0}}(f_{v_{0}}).

For the ”only if” part, we just need to use Proposition 6.11, since for (7.3.1) to be true, by assumption, the only ingredient we need is simply SOδv0θG¯(E¯v0)(ϕv0)=SOγv0G¯(F¯v0)(fv0)SO^{\underline{G}(\underline{E}_{v_{0}})}_{\delta_{v_{0}}\theta}(\phi_{v_{0}})=SO^{\underline{G}(\underline{F}_{v_{0}})}_{\gamma_{v_{0}}}(f_{v_{0}}) for every γ=𝒩δ\gamma=\mathcal{N}\delta, which holds by assumption. ∎

Proposition 7.3.

Local data adapted to Irrχ,λ(G)\mathrm{Irr}_{\chi,\lambda}(G) in the sense of §7.1 exists.

Proof.

On the spectral side, we can rewrite equation (7.3.1) as

ΠtrΠIθ,ϕ=cπtrπ,f,\sum_{\Pi}\langle\text{tr}\,\Pi I_{\theta},\phi\rangle=c\sum_{\pi}\langle\text{tr}\,\pi,f\rangle,

where the sum is over automorphic cuspidal representations Π\Pi (resp., π\pi) in the decomposition of the space Lcusp2(H¯(E¯)\H¯(𝔸E¯),λ)L^{2}_{\text{cusp}}(\underline{H}(\underline{E})\backslash\underline{H}(\mathbb{A}_{\underline{E}}),\lambda) (resp., Lcusp2(H¯(F¯)\H¯(𝔸F¯),λ)L^{2}_{\text{cusp}}(\underline{H}(\underline{F})\backslash\underline{H}(\mathbb{A}_{\underline{F}}),\lambda)). Using the product decomposition of ϕ\phi and ff, this is

(7.3.2) ΠvtrΠvIθ,ϕv=cπvtrπv,fv\sum_{\Pi}\prod_{v}\langle\text{tr}\,\Pi_{v}I_{\theta},\phi_{v}\rangle=c\sum_{\pi}\prod_{v}\langle\text{tr}\,\pi_{v},f_{v}\rangle

Therefore the identity (7.3.1) is equivalent to the identity (7.3.2). Fixing the functions ϕv,fv\phi_{v},f_{v} at the places other than v0v_{0}, for each we get an identity

ΠtrΠv0Iθ,ϕv0trΠv0Iθ,ϕv0=πtrπv0,fv0trπv0,fv0.\sum_{\Pi}\langle\text{tr}\,\Pi^{v_{0}}I_{\theta},\phi^{v_{0}}\rangle\langle\text{tr}\,\Pi_{v_{0}}I_{\theta},\phi_{v_{0}}\rangle=\sum_{\pi}\langle\text{tr}\,\pi^{v_{0}},f^{v_{0}}\rangle\langle\text{tr}\,\pi_{v_{0}},f_{v_{0}}\rangle.

Assuming fv0f_{v_{0}} and ϕv0\phi_{v_{0}} range only over functions bi-ρ\rho-invariant under a fixed Iwahori subgroup, then at v0v_{0}, the function is bi-invariant under the pro-unipotent of that fixed Iwahori subgroup, outside of v0v_{0}, the functions must be biinvariant under certain open compact subgroup ([16], Lemma 5.2.1). That is to say, the level at all places are fixed. Therefore, we can just apply an adapted version of Harish-Chandra’s finiteness theorem (Lemma 7.4) for cusp forms to see that, the number of representations Π\Pi (resp. π\pi) make nonzero contribution to the above identity is finite.

Since the sums that we want ultimately in the local data are over automorphic representations of local component at v0v_{0}, we regroup the summation as

(7.3.3) Πv0[Π s.t.Πv0Πv0trΠv0Iθ,ϕv0]trΠv0Iθ,ϕv0=πv0[π s.t.πv0πv0trπv0,fv0]trπv0,fv0.\sum_{\Pi_{v_{0}}}[\sum_{\begin{subarray}{c}\Pi^{\prime}\text{ s.t.}\\ \Pi^{\prime}_{v_{0}}\cong\Pi_{v_{0}}\end{subarray}}\langle\text{tr}\,\Pi^{\prime v_{0}}I_{\theta},\phi^{v_{0}}\rangle]\langle\text{tr}\,\Pi_{v_{0}}I_{\theta},\phi_{v_{0}}\rangle=\sum_{\pi_{v_{0}}}[\sum_{\begin{subarray}{c}\pi^{\prime}\text{ s.t.}\\ \pi^{\prime}_{v_{0}}\cong\pi_{v_{0}}\end{subarray}}\langle\text{tr}\,\pi^{\prime v_{0}},f^{v_{0}}\rangle]\langle\text{tr}\,\pi_{v_{0}},f_{v_{0}}\rangle.

Where the outer sums are over isomorphic classes of irreducible cuspidal (θ\theta-stable) automorphic representations of G¯(E¯v0)\underline{G}(\underline{E}_{v_{0}}) (resp. G¯(F¯v0)\underline{G}(\underline{F}_{v_{0}})) that transforms under the central character λr,v01\lambda^{-1}_{r,v_{0}} (resp. λv01\lambda_{v_{0}}^{-1}). In particular, they are in Irrχr,v0,λr,v0θ(G¯(E¯v0))\text{Irr}^{\theta}_{\chi_{r,v_{0}},\lambda_{r,v_{0}}}(\underline{G}(\underline{E}_{v_{0}})) (resp. Irrχv0,λv0θ(G¯(F¯v0))\text{Irr}^{\theta}_{\chi_{v_{0}},\lambda_{v_{0}}}(\underline{G}(\underline{F}_{v_{0}}))). Now we set

b(Πv0)=Π s.t.Πv0Πv0trΠv0Iθ,ϕv0a(πv0)=π s.t.πv0πv0trπv0,fv0\begin{split}b(\Pi_{v_{0}})&=\sum_{\begin{subarray}{c}\Pi^{\prime}\text{ s.t.}\\ \Pi^{\prime}_{v_{0}}\cong\Pi_{v_{0}}\end{subarray}}\langle\text{tr}\,\Pi^{\prime v_{0}}I_{\theta},\phi^{v_{0}}\rangle\\ a(\pi_{v_{0}})&=\sum_{\begin{subarray}{c}\pi^{\prime}\text{ s.t.}\\ \pi^{\prime}_{v_{0}}\cong\pi_{v_{0}}\end{subarray}}\langle\text{tr}\,\pi^{\prime v_{0}},f^{v_{0}}\rangle\end{split}

Then (7.3.3) becomes

(7.3.4) Πv0b(Πv0)trΠv0Iθ,ϕv0=πv0a(πv0)trπv0,fv0,\sum_{\Pi_{v_{0}}}b(\Pi_{v_{0}})\langle\text{tr}\,\Pi_{v_{0}}I_{\theta},\phi_{v_{0}}\rangle=\sum_{\pi_{v_{0}}}a(\pi_{v_{0}})\langle\text{tr}\,\pi_{v_{0}},f_{v_{0}}\rangle,

therefore, the implication (B)\Rightarrow(A) in the definition of local data is proved.

Assume that (7.3.4) holds for the functions ϕv0\phi_{v_{0}} and fv0f_{v_{0}}, since we already fix functions at other places vv other than v0v_{0}, we get (7.3.3), thus (7.3.2), ultimately (7.3.1). Then we get ϕv0\phi_{v_{0}} and fv0f_{v_{0}} are associated at strongly regular norms by Proposition 7.2, hence the implication (A)\Rightarrow(B) is also proved. ∎

Lemma 7.4.

(Harish-Chandra’s finiteness Theorem for cusp forms over function fields) Let KK be an open compact subgroup of G¯(𝔸F¯)\underline{G}(\mathbb{A}_{\underline{F}}), let Vcusp(λ,K)V_{\mathrm{cusp}}(\lambda,K) denote the space of cuspidal functions f:G¯(F)\G¯(𝔸F¯)/Kf:\underline{G}(F)\backslash\underline{G}(\mathbb{A}_{\underline{F}})/K\to\mathbb{C} such that f(zg)=λ(z)f(g)f(zg)=\lambda(z)f(g) for all gZ¯(𝔸F¯)g\in\underline{Z}(\mathbb{A}_{\underline{F}}). Then:

  1. (1)

    There exists a compact subset CG¯(𝔸F¯)C\subset\underline{G}(\mathbb{A}_{\underline{F}}) such that every function in Vcusp(λ,K)V_{\mathrm{cusp}}(\lambda,K) is supported on Z¯(𝔸F¯)G¯(F)C\underline{Z}(\mathbb{A}_{\underline{F}})\underline{G}(F)C.

  2. (2)

    dimVcusp(λ,K)<\dim V_{\mathrm{cusp}}(\lambda,K)<\infty.

Proof.

For (i), see [20] Theorem 1.2.1, also [16] Theorem 9.5.1. (ii) follows from (i) by noticing that the value of such fVcusp(λ,K)f\in V_{\text{cusp}}(\lambda,K) is determined on the finite cosets C/KC/K (we can always enlarge CC to contain KK). ∎

7.4. A Further Reduction

In this subsection, we show that the existence of local data adapted to Irrχ,λ(G)\mathrm{Irr}_{\chi,\lambda}(G) for all unitary characters λ\lambda implies the existence of local data adapted to Irrχ(G)\mathrm{Irr}_{\chi}(G), so that we are back to the scenario considered in [19]. The local data adapted to Irrχ(G)\text{Irr}_{\chi}(G) is given analogously as follows:

  1. (1)

    An indexing set \mathcal{I}, possibly infinite;

  2. (2)

    A collection of complex numbers ai(π)a_{i}(\pi) for ii\in\mathcal{I} and πIrrχ(G)\pi\in\text{Irr}_{\chi}(G);

  3. (3)

    A collection of complex numbers bi(Π)b_{i}(\Pi) for ii\in\mathcal{I} and ΠIrrχrθ(Gr)\Pi\in\text{Irr}^{\theta}_{\chi_{r}}(G_{r}).

  1. (1)

    For ii fixed, the constants ai(π)a_{i}(\pi) and bi(Π)b_{i}(\Pi) are zero for all but finitely many π\pi and Π\Pi.

  2. (2)

    For ϕ(Gr,ρr)\phi\in\mathcal{H}(G_{r},\rho_{r}) and f(G,ρ)f\in\mathcal{H}(G,\rho), the following statements are equivalent:

    1. (a)

      For all ii, we have πai(π)trπ,f=Πbi(Π)trΠIθ,ϕ\sum_{\pi}a_{i}(\pi)\langle\text{tr}\,\pi,f\rangle=\sum_{\Pi}b_{i}(\Pi)\langle\text{tr}\,\Pi I_{\theta},\phi\rangle;

    2. (b)

      For all strongly regular elliptic semisimple norms γ=𝒩(δ)\gamma=\mathcal{N}(\delta), we have

      SOγ(f)=SOδθ(ϕ).SO_{\gamma}(f)=SO_{\delta\theta}(\phi).
Proposition 7.5.

Assume local data adapted to Irrχ,λ(G)\mathrm{Irr}_{\chi,\lambda}(G) exists for all unitary character λ\lambda on ZZ, then the local data adapted to Irrχ(G)\mathrm{Irr}_{\chi}(G) exists.

Proof.

Indeed, given that local data exists for every unitary character λ\lambda, denote λ\mathcal{I}_{\lambda} to be the index set in the corresponding local data, we take =λλ\mathcal{I}=\displaystyle\coprod_{\lambda}\mathcal{I}_{\lambda}. For πIrrχ(G)\pi\in\mathrm{Irr}_{\chi}(G), if πIrrχ,λ(G)\pi\in\mathrm{Irr}_{\chi,\lambda}(G), then we take ai(π)a_{i}(\pi) to be the complex number in the local data adapted to Irrχ,λ(G)\mathrm{Irr}_{\chi,\lambda}(G), otherwise we set ai(π)=0a_{i}(\pi)=0. We set complex numbers bi(Π)b_{i}(\Pi) analogously. Therefore we have data (a’), (b’), (c’), subject to condition (1’).

If (2’)(A’) is satisfied, for any character λ\lambda and all iλi\in\mathcal{I}_{\lambda}, we have

πai(π)trπ,f=Πbi(Π)trΠIθ,ϕ.\displaystyle\sum_{\pi}a_{i}(\pi)\langle\text{tr}\,\pi,f\rangle=\sum_{\Pi}b_{i}(\Pi)\langle\text{tr}\,\Pi I_{\theta},\phi\rangle.

It is straightforward to check that for πIrrχ,λ(G)\pi\in\text{Irr}_{\chi,\lambda}(G) (resp. ΠIrrχr,λr(Gr)\Pi\in\text{Irr}_{\chi_{r},\lambda_{r}}(G_{r})), we have trπ,f=trπ,fλ\langle\text{tr}\,\pi,f\rangle=\langle\text{tr}\,\pi,f_{\lambda}\rangle (resp. trΠIθ,ϕ=trΠIθ,ϕλr\langle\text{tr}\,\Pi I_{\theta},\phi\rangle=\langle\text{tr}\,\Pi I_{\theta},\phi_{\lambda_{r}}\rangle ) (recall that the latter traces are defined over G/ZG/Z). Therefore, we have (fλ,ϕλr)(f_{\lambda},\phi_{\lambda_{r}}) are associated for any unitary character λ\lambda on ZZ. By Lemma 4.4 (i) and the further reduction to unitary characters, we can assert that (2’)(B’) holds.

Similarly if (2’)(B’) is satisfied, we just reverse the process above to get (2’)(A’). Therefore we have the existence of local data adapted to Irrχ(G)\text{Irr}_{\chi}(G).

7.5. Labesse elementary functions and their traces

We collect the definitions and properties of Labesse elementary functions that were defined and used in [19] in this subsection. They will be used to prove (2’)(A’).

Recall that AFrA^{F_{r}} is a maximal FrF_{r}-split torus in GG, whose centralizer TT is a maximal FF-torus. Let B=TUB=TU be the FF-rational Borel subgroup defining the dominant Weyl chamber in X(A)X_{*}(A)_{\mathbb{R}}. Let ρ\rho denote the half-sum of the BB-positive roots of GG.

We fix a uniformizer ϖ\varpi for the field FF. We have the following commutative diagram:

X(AFr){\lx@inpgf@ignorespaces X_{*}(A^{F_{r}})}T(Fr){\lx@inpgf@ignorespaces T(F_{r})}X(A){\lx@inpgf@ignorespaces X_{*}(A)}T(F){\lx@inpgf@ignorespaces T(F)}(ϖ)\scriptstyle{\lx@inpgf@ignorespaces\cdot(\varpi)}Nr\scriptstyle{\lx@inpgf@ignorespaces N_{r}}Nr\scriptstyle{\lx@inpgf@ignorespaces N_{r}}(ϖ)\scriptstyle{\lx@inpgf@ignorespaces\cdot(\varpi)}

Consider a regular dominant cocharacter νX(AFr)\nu\in X_{*}(A^{F_{r}}) and set u=ν(ϖ)T(Fr)u=\nu(\varpi)\in T(F_{r}). Therefore we have τ=Nr(ν)\tau=N_{r}(\nu) is also a regular dominant cocharacter in X(A)X_{*}(A) with t=τ(ϖ)=Nr(u)T(F)t=\tau(\varpi)=N_{r}(u)\in T(F). Labesse[42] constructed FF-rational parabolic subgroup PuθP_{u\theta} with FF-rational unipotent radical NuθN_{u\theta} and FF-rational Levi factor MuθM_{u\theta} to uθGrθu\theta\in G_{r}\rtimes\langle\theta\rangle. The subgroups MuθM_{u\theta} (resp. PuθP_{u\theta}) of GG can be characterized as the set of elements gGg\in G such that (uθ)ng(uθ)n(u\theta)^{n}g(u\theta)^{-n} remains bounded as nn ranges over all integers (resp. all positive integers). Since (uθ)r=t(u\theta)^{r}=t, we have Muθ=Mt=TM_{u\theta}=M_{t}=T and Puθ=Pt=BP_{u\theta}=P_{t}=B.

Consider the map

(7.5.1) T(Fr)1\Ir×T(Fr)1uGr[k,mu]k1muθ(k)\begin{split}T(F_{r})_{1}\backslash I_{r}\times T(F_{r})_{1}u&\to G_{r}\\ [k,mu]&\mapsto k^{-1}mu\theta(k)\end{split}

where [k,mu][k,mu] denotes the equivalent class of (k,mu)Ir×T(Fr)1u(k,mu)\in I_{r}\times T(F_{r})_{1}u under the action of m0T(Fr)1m_{0}\in T(F_{r})_{1} by m0(k,mu)=(m0k,m0muθ(m0)1)m_{0}\cdot(k,mu)=(m_{0}k,m_{0}mu\theta(m_{0})^{-1}). This map is injective whose image is a compact open subset 𝔏uGr\mathfrak{L}_{u}\subset G_{r}.

Definition 7.6.

We define the elementary function ϕu,χr\phi_{u,\chi_{r}} on GrG_{r} to vanish off of 𝔏u\mathfrak{L}_{u}, and on 𝔏u\mathfrak{L}_{u}, it is given by

ϕu,χr(k1muθ(k))=χr1(m)\phi_{u,\chi_{r}}(k^{-1}mu\theta(k))=\chi^{-1}_{r}(m)

for kIrk\in I_{r} and mT(Fr)1m\in T(F_{r})_{1}.

We summarize the useful properties of ϕu,χr\phi_{u,\chi_{r}} in the following proposition.

Proposition 7.7.
  1. (1)

    The functions ϕu,χr\phi_{u,\chi_{r}} are well-defined and belong to (Gr,ρr)\mathcal{H}(G_{r},\rho_{r}).

  2. (2)

    The functions ϕu,χr\phi_{u,\chi_{r}} are supported on the set of strongly θ\theta-regular elements in GrG_{r}.

Proof.

(2) is from Lemma 8.1.2 (ii) in [19]. For (1), the fact that the functions are well-defined is easy to check. To show that they belong to the Hecke algebra, the first step is to show that 𝔏u=IruIr\mathfrak{L}_{u}=I_{r}uI_{r}. It is clear that 𝔏uIruIr\mathfrak{L}_{u}\subset I_{r}uI_{r} by 7.5.1. To show the equality, following [43] Prop. IV.1.1, since both sides are open compact, it suffices to show that they have the same volume. It is straightforward to see that they are of the same volume vol(Ir)vol(Ir/uIru1)=vol(Ir)δBr1(u)\mathrm{vol}(I_{r})\cdot\mathrm{vol}(I_{r}/uI_{r}u^{-1})=\mathrm{vol}(I_{r})\cdot\delta^{-1}_{B_{r}}(u). To show that it is in the Hecke algebra, the calculations in the proof of [19] Lemma 8.1.3 is still valid here. ∎

When r=1r=1 and u=tu=t, we can define ft,χ(G,ρ)f_{t,\chi}\in\mathcal{H}(G,\rho) analogously. By §8.3 in [19], we have the following associated results:

Proposition 7.8.

The functions ft,χf_{t,\chi} and ϕu,χr\phi_{u,\chi_{r}} are associated.

The next step is to calculate the traces of elementary functions. Let Π\Pi denote a θ\theta-stable admissible representation of GrG_{r}, and fix an intertwiner Iθ:ΠΠθI_{\theta}:\Pi\cong\Pi^{\theta}. The locally integrability of the distribution character in characteristic 00 that was used in §8.4-8.5 in [19] is also available in the restricted form by Proposition 13.1 of [3]:

Proposition 7.9.

For ϕCc(Gθreg(Fr))\phi\in C^{\infty}_{c}(G^{\theta\mathrm{-reg}}(F_{r})), where Gθreg(Fr)G^{\theta\mathrm{-reg}}(F_{r}) is the open subset of θ\theta-regular elements in G(Fr)G(F_{r}) whose complement has measure 00, the functional ϕtrΠIθ,ϕ\phi\mapsto\langle\mathrm{tr}\,\Pi I_{\theta},\phi\rangle is represented by a locally constant function ΘΠθ\Theta_{\Pi\theta} on Gθreg(Fr)G^{\theta\mathrm{-reg}}(F_{r}). That is,

(7.5.2) trΠIθ,ϕ=GrΘΠθ(g)ϕ(g)𝑑g\langle\mathrm{tr}\,\Pi I_{\theta},\phi\rangle=\int_{G_{r}}\Theta_{\Pi\theta}(g)\phi(g)\,dg

The fact that our elementary functions are supported inside the set of θ\theta-regular elements (Proposition 7.7 (2)) allows us to repeat the same calculations as in [19]. Along the way, we also use the twisted trace identity ΘΠθ(mu)=ΘΠUθ(mu)\Theta_{\Pi\theta}(mu)=\Theta_{\Pi_{U}\theta}(mu) of Rogawski ([50], Prop. 7.4), where ΠU\Pi_{U} is the Jacquet module of Π\Pi corresponding to the Borel subgroup Br=TrUrB_{r}=T_{r}U_{r}.

We fix some notations before we get into the traces of elementary functions. We write WW (resp. WrW_{r}) for the relative Weyl group associated to the FF-split (resp. FrF_{r}-split) torus AA (resp. AFrA^{F_{r}}) in GG.

  • Let Ξ\Xi denote the set of characters on T(Fr)T(F_{r}) which extend some WrW_{r}-conjugate of χr\chi_{r}. Let Ξ(χr)Ξ\Xi(\chi_{r})\subset\Xi consist of those whose restriction to T(Fr)1T(F_{r})_{1} is precisely χr\chi_{r}. For ξΞ(χr)\xi^{\prime}\in\Xi(\chi_{r}), we may write

    ξ=χ~rϖη\xi^{\prime}=\tilde{\chi}^{\varpi}_{r}\eta^{\prime}

    for a unique unramified character η\eta^{\prime} on TrT_{r} (see Remark 3.4 for the definition of χ~rϖ\tilde{\chi}^{\varpi}_{r}).

  • Let Ξθ\Xi^{\theta} (resp. Ξ(χr)θ\Xi(\chi_{r})^{\theta}) denote the subset of θ\theta-fixed elements in Ξ\Xi (resp. Ξ(χr)\Xi(\chi_{r})).

Suppose the supercuspidal support of Π\Pi is (Tr,ξ)Gr(T_{r},\xi^{\prime})_{G_{r}} for some extension ξ\xi^{\prime} of a WrW_{r}-conjugate of χr\chi_{r}. Then ΠU\Pi_{U} is a subquotient of

(iBrGr(ξ))U=δBr1/2wWrξw(i^{G_{r}}_{B_{r}}(\xi^{\prime}))_{U}=\delta^{1/2}_{B_{r}}\bigoplus_{w\in W_{r}}\mathbb{C}_{{}^{w}\xi^{\prime}}

(cf. [6], Prop. 6.4.1), where ξw\mathbb{C}_{{}^{w}\xi^{\prime}} is the character on TrT_{r} corresponding to ξw{}^{w}\xi^{\prime}.

  • We have a well-defined subset Ξ(Π)Ξ\Xi(\Pi)\subset\Xi and positive multiplicities aξa_{\xi^{\prime}} for ξΞ(Π)\xi\in\Xi(\Pi) such that

    ΠU=δBr1/2wΞ(Π)ξaξ\Pi_{U}=\delta^{1/2}_{B_{r}}\bigoplus_{w\in\Xi(\Pi)}\mathbb{C}^{a_{\xi^{\prime}}}_{\xi^{\prime}}
  • Set Ξ(Π)θ=ΞθΞ(Π)\Xi(\Pi)^{\theta}=\Xi^{\theta}\cap\Xi(\Pi) and Ξ(Π,χr)θ=Ξ(χr)θΞ(Π)\Xi(\Pi,\chi_{r})^{\theta}=\Xi(\chi_{r})^{\theta}\cap\Xi(\Pi).

  • For ξΞθ\xi^{\prime}\in\Xi^{\theta}, we set

    tr(Iθ,Π,ξ):=trIθ;δBr1/2ξaξ.\mathrm{tr}(I_{\theta},\Pi,\xi^{\prime}):=\langle\mathrm{tr}\,I_{\theta};\delta^{1/2}_{B_{r}}\mathbb{C}^{a_{\xi^{\prime}}}_{\xi^{\prime}}\rangle.

    Here we recall that the intertwiner Iθ:ΠΠθI_{\theta}:\Pi\cong\Pi^{\theta} induces an intertwiner Iθ:ΠUΠUθI_{\theta}:\Pi_{U}\cong\Pi^{\theta}_{U}.

We summarize the traces of elementary functions in the following proposition.

Proposition 7.10.
  1. (1)

    Suppose Π\Pi is an irreducible and θ\theta-stable object in (Gr)\mathfrak{R}(G_{r}). If
    trΠIθ,ϕu,χr0\langle\mathrm{tr}\,\Pi I_{\theta},\phi_{u,\chi_{r}}\rangle\neq 0, then Πχr(Gr)\Pi\in\mathfrak{R}_{\chi_{r}}(G_{r}).

  2. (2)

    For Πχr(Gr)\Pi\in\mathfrak{R}_{\chi_{r}}(G_{r}), we have

    (7.5.3) trΠIθ,ϕu,χr=qρ,τξΞ(Π,χr)θη(u)tr(Iθ,Π,ξ).\langle\mathrm{tr}\,\Pi I_{\theta},\phi_{u,\chi_{r}}\rangle=q^{\langle\rho,\tau\rangle}\sum_{\xi^{\prime}\in\Xi(\Pi,\chi_{r})^{\theta}}\eta^{\prime}(u)\mathrm{tr}(I_{\theta},\Pi,\xi^{\prime}).

    In particular, when r=1r=1, we have

    (7.5.4) trπ,ft,χ=qρ,τξΞ(π,χ)η(t)dimξaξ.\langle\mathrm{tr}\,\pi,f_{t,\chi}\rangle=q^{\langle\rho,\tau\rangle}\sum_{\xi^{\prime}\in\Xi(\pi,\chi)}\eta(t)\dim\mathbb{C}^{a_{\xi}}_{\xi}.
  3. (3)

    Let eρr𝒵(Gr,ρr)e_{\rho_{r}}\in\mathcal{Z}(G_{r},\rho_{r}) be the idempotent to have support II and to take value ρr(k)1\rho_{r}(k)^{-1} at kIrk\in I_{r}. Then we have

    (7.5.5) trΠIθ,eρr=ξΞ(Π,χr)θtr(Iθ,Π,ξ),\langle\mathrm{tr}\,\Pi I_{\theta},e_{\rho_{r}}\rangle=\sum_{\xi^{\prime}\in\Xi(\Pi,\chi_{r})^{\theta}}\mathrm{tr}(I_{\theta},\Pi,\xi^{\prime}),

    and

    (7.5.6) trΠIθ,eρr=trΠIθ,ϕu,χr|u=1.\langle\mathrm{tr}\,\Pi I_{\theta},e_{\rho_{r}}\rangle=\langle\mathrm{tr}\,\Pi I_{\theta},\phi_{u,\chi_{r}}\rangle|_{u=1}.

    In particular, when r=1r=1, we have

    (7.5.7) trπ,eρ=ξΞ(π,χ)dimξaξ.\langle\mathrm{tr}\,\pi,e_{\rho}\rangle=\sum_{\xi^{\prime}\in\Xi(\pi,\chi)}\dim\mathbb{C}^{a_{\xi}}_{\xi}.
Proof.

The calculations in the proof of Lemma 8.4.1 and §8.5 in [19] carry over unchanged. ∎

7.6. End of Proof

We fix ϕZ(Gr,ρr)\phi\in Z(G_{r},\rho_{r}) and f=b(ϕ)𝒵(G,ρ)f=b(\phi)\in\mathcal{Z}(G,\rho). By the various reduction steps, we may assume γ\gamma is a (strongly) regular elliptic semisimple norm, i.e., γ=𝒩(δ)\gamma=\mathcal{N}(\delta) for some δG(E)\delta\in G(E) θ\theta-(strongly) regular θ\theta-elliptic semisimple. Proposition 7.5 guarantees that we are in the situation considered in [19], §9.2. Thus by Proposition 7.8, we have

(7.6.1) πai(π)trπ,ft=Πbi(Π)trΠIθ,ϕu\sum_{\pi}a_{i}(\pi)\langle\text{tr}\,\pi,f_{t}\rangle=\sum_{\Pi}b_{i}(\Pi)\langle\text{tr}\,\Pi I_{\theta},\phi_{u}\rangle

for each pair of functions (ft,ϕu)(f_{t},\phi_{u}), where we denote ft:=ft,χf_{t}:=f_{t,\chi} and ϕu:=ϕu,χr\phi_{u}:=\phi_{u,\chi_{r}}. As in loc. cit., we can eventually separate (7.6.1) into

(7.6.2) ξ0Ξ(χ)/Wχs.t. ξ0rWχrξ0πiBG(ξ0)a(π)trπ,eρ=ΠiBrGr(ξ0)b(Π)trΠIθ,eρr\begin{split}\sum_{\begin{subarray}{c}\xi_{0}\in\Xi(\chi)/W_{\chi}\\ \text{s.t. }\xi_{0r}\in W_{\chi_{r}}\xi^{\prime}_{0}\end{subarray}}\sum_{\pi\in i^{G}_{B}(\xi_{0})}a(\pi)&\langle\text{tr}\,\pi,e_{\rho}\rangle=\\ &\sum_{\Pi\in i^{G_{r}}_{B_{r}}(\xi^{\prime}_{0})}b(\Pi)\,\langle\text{tr}\,\Pi I_{\theta},e_{\rho_{r}}\rangle\end{split}

for a fixed ξ0Ξ(χr)θ\xi^{\prime}_{0}\in\Xi(\chi_{r})^{\theta} where both sides will vanish if Wχrξ0W_{\chi_{r}}\xi^{\prime}_{0} contains no norm. If ξ0=ξ0r\xi^{\prime}_{0}=\xi_{0r}, we multiply both sides of (7.6.2) by chξ0(b(ϕ))=chξ0r(ϕ)ch_{\xi_{0}}(b(\phi))=ch_{\xi_{0r}}(\phi), if ξ0\xi^{\prime}_{0} is not a norm, we multiply both sides of (7.6.2) by chξ0(ϕ)ch_{\xi^{\prime}_{0}}(\phi). The upshot is that, after summing over ξ0Ξ(χr)/Wχr\xi^{\prime}_{0}\in\Xi(\chi_{r})/W_{\chi_{r}}, we will have the desired identities of traces

(7.6.3) πai(π)trπ,b(ϕ)=Πbi(Π)trΠIθ,ϕ.\sum_{\pi}a_{i}(\pi)\langle\text{tr}\,\pi,b(\phi)\rangle=\sum_{\Pi}b_{i}(\Pi)\langle\text{tr}\,\Pi I_{\theta},\phi\rangle.

Therefore ϕ\phi and b(ϕ)b(\phi) are associated at all strongly regular elliptic elements, as desired.

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