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Shelstad’s character identity from the point of view of index theory

Peter Hochs111University of Adelaide, peter.hochs@adelaide.edu.au  and Hang Wang222University of Adelaide, hang.wang01@adelaide.edu.au
(September 13, 2025)
Abstract

Shelstad’s character identity is an equality between sums of characters of tempered representations in corresponding LL-packets of two real, semisimple, linear, algebraic groups that are inner forms to each other. We reconstruct this character identity in the case of the discrete series, using index theory of elliptic operators in the framework of KK-theory. Our geometric proof of the character identity is evidence that index theory can play a role in the classification of group representations via the Langlands program.

1 Introduction

The aim of this paper is to use our previous results in [HW2] to compare representations of two connected real semisimple groups G,GG,G^{\prime} having the same Langlands dual group. We are inspired by the so-called Shelstad’s character identity following from Langlands program [S1, S2]. In fact, in the local Langlands program [L1, L2, L3], every admissible representation of a real reductive Lie group is labeled by its LL-parameter, which is represented by a homomorphism from the Weil group WW_{\mathbb{R}} of the real numbers to the Langlands dual group of G.G. If two real reductive groups GG and GG^{\prime} have the same Langlands dual group, then every LL-parameter ϕ\phi of GG can be identified to an LL-parameter ϕ\phi^{\prime} for GG^{\prime}. Denote by Πϕ\Pi_{\phi} the LL-packet of ϕ\phi, i.e., the set of admissible representations of GG having the same LL-parameter ϕ\phi. Shelstad’s character identity states that the characters Θπ\Theta_{\pi} of tempered representations π\pi for GG and GG^{\prime} associated to the same LL-parameter satisfy the identity

(1)dimG/KπΠϕΘπ(h)=(1)dimG/KπΠϕΘπ(h),(-1)^{\dim G/K}\sum_{\pi\in\Pi_{\phi}}\Theta_{\pi}(h)=(-1)^{\dim G^{\prime}/K^{\prime}}\sum_{\pi^{\prime}\in\Pi_{\phi^{\prime}}}\Theta_{\pi^{\prime}}(h^{\prime}), (1.1)

if hh and hh^{\prime} are corresponding regular elements of Cartan subgroups H<GH<G and H<GH^{\prime}<G^{\prime}, respectively.

The main result of this paper is a direct geometric proof of the character identity (1.1) in the case of discrete series representations, without referring to character formulas or the theory of Langlands program. The proof uses index theory and KK-theory of CC^{*}-algebras, and illustrates how these are related to representation theory and the Langlands program.

Acknowledgements

The authors are grateful to Kuok Fai Chao for background information about the Langlands program. The second author was supported by the Australian Research Council, through Discovery Early Career Researcher Award DE160100525.

2 Character identities and index theory

2.1 Inner forms

We recall the definition of inner forms, as discussed for example in [ABV]. Let GG_{\mathbb{C}} be a connected reductive complex algebraic group. A real form of GG_{\mathbb{C}} is an involutive automorphism σ:GG\sigma\colon G_{\mathbb{C}}\rightarrow G_{\mathbb{C}} which is antiholomorphic; i.e., Teσ(iX)=iTeσ(X)T_{e}\sigma(iX)=-iT_{e}\sigma(X) for all X𝔤X\in\mathfrak{g}_{\mathbb{C}}. The involution σ\sigma is a generalised notion of complex conjugation. The group of real points of σ\sigma

G(,σ)={gG:σ(g)=g}G(\mathbb{R},\sigma)=\{g\in G_{\mathbb{C}}:\sigma(g)=g\}

is called the real form of GG_{\mathbb{C}} associated to σ.\sigma.

Definition 2.1 ([ABV, Chapter 2]).

Two real forms G(,σ)G(\mathbb{R},\sigma) and G(,σ)G(\mathbb{R},\sigma^{\prime}) of GG_{\mathbb{C}} are said to be inner to each other if there is an element gGg\in G_{\mathbb{C}} such that

σ=Cgσ,\sigma^{\prime}=C_{g}\circ\sigma, (2.1)

where CgC_{g} denotes conjugation by gg. The real group G:=G(,σ)G^{\prime}:=G(\mathbb{R},\sigma^{\prime}) is called an inner form of the real group G:=G(,σ)G:=G(\mathbb{R},\sigma).

The set of inner forms for GG can be identified bijectively to the first Galois cohomology H1(Γ,Inn(G))H^{1}(\Gamma,\operatorname{Inn}(G_{\mathbb{C}})) where Γ\Gamma is the Galois group Gal(/)\operatorname{Gal}(\mathbb{C}/\mathbb{R}) of two elements, where the complex conjugation (the generator) takes ηAut(G)\eta\in\operatorname{Aut}(G_{\mathbb{C}}) to σησ1Aut(G)\sigma\circ\eta\circ\sigma^{-1}\in\operatorname{Aut}(G_{\mathbb{C}}), and Inn(G)\operatorname{Inn}(G_{\mathbb{C}}) is the subgroup of inner automorphisms of GG_{\mathbb{C}} respecting the action of Γ\Gamma. See [B].

Example 2.2.
  • Let G=SL(2,)G_{\mathbb{C}}=\operatorname{SL}(2,\mathbb{C}). GG_{\mathbb{C}} has a compact real form G=SU(2)G=\operatorname{SU}(2) associated to σ(g)=(g¯T)1\sigma(g)=(\bar{g}^{T})^{-1} and a split real form G=SL(2,)G^{\prime}=\operatorname{SL}(2,\mathbb{R}) accosiated to σ(g)=g¯.\sigma(g)=\bar{g}. It can be checked that GG^{\prime} is the unique inner form for GG.

  • SL(n,)\operatorname{SL}(n,\mathbb{R}) when nn odd does not have any inner form other than itself; It has an extra inner form if nn is even. Note that when n3n\geq 3, SL(n,)\operatorname{SL}(n,\mathbb{R}) does not have compact inner forms in view of Theorem 2.5 below.

  • U(2)\operatorname{U}(2) and U(1,1)\operatorname{U}(1,1) are inner forms to each other.

  • SU(2,1)\operatorname{SU}(2,1) and SU(3)\operatorname{SU}(3) are inner forms to each other.

  • SO(2p,2q)\operatorname{SO}(2p,2q) where 2p+2q=4n2p+2q=4n are inner forms to each other. In particular, SO(4n)\operatorname{SO}(4n) is the compact inner form amongst elements of this set.

If GG and GG^{\prime} are inner forms to each other in a complex group GG_{\mathbb{C}}, then any Cartan subgroup H<GH<G is conjugate in GG_{\mathbb{C}} to a Cartan subgroup H<GH^{\prime}<G^{\prime}. See Lemma 2.1 of [L3] and [S2]. We will use this to identify elements hHh\in H to corresponding elements hHh^{\prime}\in H^{\prime}.

Example 2.3.

Let G=SU(2)G=\operatorname{SU}(2) and G=SL(2,)G^{\prime}=\operatorname{SL}(2,\mathbb{R}). Then their respective Cartan subgroups

T={[eiθ00eiθ]:θ}andT={[cosθsinθsinθcosθ]:θ}T=\left\{\begin{bmatrix}e^{i\theta}&0\\ 0&e^{-i\theta}\end{bmatrix}:\theta\in\mathbb{R}\right\}\qquad\text{and}\qquad T^{\prime}=\left\{\begin{bmatrix}\cos\theta&\sin\theta\\ -\sin\theta&\cos\theta\end{bmatrix}:\theta\in\mathbb{R}\right\}

are conjugated by [i112i2]SL(2,).\begin{bmatrix}-i&-1\\ \frac{1}{2}&\frac{i}{2}\end{bmatrix}\in\operatorname{SL}(2,\mathbb{C}).

2.2 LL-packets and character identities

Inner forms are closely related to the Langlands program. Let GG be a real reductive algebraic group, and let GG^{\vee} denote the Langlands dual group of GG. Consider the LL-group GL=GGal(/){}^{L}\!G=G^{\vee}\rtimes\operatorname{Gal}(\mathbb{C}/\mathbb{R}). Let WW_{\mathbb{R}} be the Weil group of real numbers, i.e., the group ×j×\mathbb{C}^{\times}\cup j\mathbb{C}^{\times} subject to relations

j2=1andjz=z¯j.j^{2}=-1\quad\text{and}\quad jz=\overline{z}j.

Then the irreducible admissible representations of GG are parametrised by LL-parameters. These are group homomorphisms

ϕ:WLG\phi\colon W_{\mathbb{R}}\rightarrow^{L}\!G

satisfying certain conditions. In fact, the local Langlands correspondence gives rise to a surjective map

f:Π(G)Φ(G)wheref:\Pi(G)\rightarrow\Phi(G)\qquad\text{where} (2.2)
Π(G)\displaystyle\Pi(G) :={equivalence classes of irreducible admissible representations of G};\displaystyle:=\{\text{equivalence classes of irreducible admissible representations of }G\};
Φ(G)\displaystyle\Phi(G) :={G-conjugacy classes of L-parameters ϕ:WLG}\displaystyle:=\{\text{$G^{\vee}$-conjugacy classes of $L$-parameters }\phi\colon W_{\mathbb{R}}\rightarrow^{L}\!G\}

where f1({ϕ})f^{-1}(\{\phi\}) is finite for every ϕΦ(G).\phi\in\Phi(G). The finite set

Πϕ:=f1({ϕ})\Pi_{\phi}:=f^{-1}(\{\phi\})

is called the LL-packet associated to the LL-parameter ϕ\phi. In other words, two admissible irreducible representations π1,π2\pi_{1},\pi_{2} are said to be in the same LL-packet if and only if they have the same LL-parameter. Representations having the same LL-parameter are indistinguishable in the sense of Langlands.

When GG and GG^{\prime} are inner forms to each other, they share the same LL-group. Groups with the same LL-group are crucial in the sense that the representation theory of these groups are closely related and can be studied globally. The character identity in Theorem 2.4 below, regarding inner forms is an instance of this philosophy. In fact, by the local Langlands correspondence, the LL-packets of admissible representations for GG and GG^{\prime} are related by their corresponding LL-parameters. Hence, a character identity involving a common LL-packet can be expected. For more details of Langlands program and character identity we refer to Langlands [L1, L2, L3] and Shelstad [S1, S2].

Let ϕ\phi be an LL-parameter of admissible representations of GG. According to Langlands [L3], all admissible representations in the same LL-packet of a tempered representation are tempered. Hence the LL-parameter ϕ\phi of a tempered representation is called tempered. Let GG^{\prime} be an inner form of GG. Suppose GG is quasi-split, meaning that GG has a σ\sigma-invariant Borel subgroup. In that case, we have Φ(G)Φ(G)\Phi(G^{\prime})\subset\Phi(G). Suppose ϕΦ(G)\phi\in\Phi(G^{\prime}). We write ϕ\phi^{\prime} for ϕ\phi, when we view it as an LL-parameter of GG^{\prime}. Then ϕ\phi^{\prime} is tempered if ϕ\phi is. The same line of statements remains true with “tempered’ replaced by “discrete series”.

For any irreducible admissible representation π\pi, we denote its global character by Θπ\Theta_{\pi}. Shelstad’s character identity is stated as follows.

Theorem 2.4 (Shelstad’s character identity [S1, S2]).

Let GG and GG^{\prime} be connected, real reductive, linear algebraic groups, and inner forms to each other in GG_{\mathbb{C}}. Suppose GG is quasi-split. Let K<GK<G and K<GK^{\prime}<G^{\prime} be maximal compact subgroups and let H<GH<G and H<GH^{\prime}<G be Cartan subgroups that are conjugate to each other in GG_{\mathbb{C}}. Let hh be an elliptic regular element of HH and hh^{\prime} the corresponding element of HH^{\prime}. Let ϕ\phi^{\prime} be a tempered LL-parameter of GG^{\prime}, and let ϕ\phi be the corresponding LL-parameter of GG. Then

(1)dimG/K2πΠϕΘπ(h)=(1)dimG/K2πΠϕΘπ(h).(-1)^{\frac{\dim G/K}{2}}\sum_{\pi\in\Pi_{\phi}}\Theta_{\pi}(h)=(-1)^{\frac{\dim G^{\prime}/K^{\prime}}{2}}\sum_{\pi^{\prime}\in\Pi_{\phi^{\prime}}}\Theta_{\pi^{\prime}}(h^{\prime}). (2.3)

This is Theorem 6.3 in [S2]. In this paper, we will prove Shelstad’s character identity (2.3) using KK-theory and index theory when Πϕ\Pi_{\phi} and Πϕ\Pi_{\phi^{\prime}} are LL-packets of discrete series representations.

2.3 Character identities for the discrete series

We now assume in addition that the group GG is semisimple, and has discrete series representations. Harish-Chandra has the following equivalent statements for existence of discrete series. See for example Theorem 22.1 in [T].

Theorem 2.5 (Harish-Chandra).

The following statements are equivalent.

  1. 1.

    GG has a compact Cartan subgroup T<GT<G;

  2. 2.

    GG has a compact inner form GG^{\prime};

  3. 3.

    GG has discrete series, i.e., square integrable representations.

In particular, if GG has a discrete series, then it always has a compact inner form.

As a result, all but the second case in Example 2.2 admit discrete series and hence they have compact Cartan subgroups. Assume GG has discrete series and TT is a compact Cartan subgroup from now on.

Theorem 2.6 ([S2, Corollary 2.9]).

Any inner form GG^{\prime} of GG also contains a compact Cartan subgroup.

So an inner form GG^{\prime} of GG also has discrete series representations.

For discrete series, we have the following property, of LL-packets, which can be found for example in [Lab].

Proposition 2.7.

If GG has discrete series, then two discrete series representations π1\pi_{1} and π2\pi_{2} are in the same LL-packet if and only if they have the same infinitesimal character.

Let K<GK<G be a maximal compact subgroup containing TT. Let WGW_{G} and WK<WGW_{K}<W_{G} be the Weyl groups of the root systems of (𝔤,𝔱)(\mathfrak{g}^{\mathbb{C}},\mathfrak{t}^{\mathbb{C}}) and (𝔨,𝔱)(\mathfrak{k}^{\mathbb{C}},\mathfrak{t}^{\mathbb{C}}), respectively. Then two discrete series representations of GG have the same infinitesimal character if and only if their Harish-Chandra parameters are in the same WGW_{G}-orbit. They are equivalent if and only if they are in the same WKW_{K}-orbit, so every discrete series LL-packet can be identified with WG/WKW_{G}/W_{K}.

In this paper, we will give a geometric proof of a special case of Theorem 2.4

Theorem 2.8.

Theorem 2.4 holds for LL-packets of discrete series representations.

This case of Theorem 2.4 can be proved by explicitly writing out Harish–Chandra’s character formula for the discrete series and rearranging terms. Our proof does not involve character formulas, and will show how this case of the character identities is related to the geometry of the space G/TG/T, and also how character identities are related to KK-theory and index theory.

Example 2.9.

Let G=SL(2,)G=\operatorname{SL}(2,\mathbb{R}), and K=T=SO(2)K=T=\operatorname{SO}(2). Let ρi𝔱\rho\in i\mathfrak{t}^{*} be the element mapping [0110]\begin{bmatrix}{0}&{-1}\\ {1}&{0}\end{bmatrix} to ii. Let nn\in\mathbb{N}, and set λ=nρ\lambda=n\rho. Let π±λG\pi^{G}_{\pm\lambda} be the discrete series representation of SL(2,)\operatorname{SL}(2,\mathbb{R}) with Harish-Chandra parameter ±λ\pm\lambda.

We have G=PGL(2,)G^{\vee}=\operatorname{PGL}(2,\mathbb{C}). The LL-parameter of the two representations π±λG\pi^{G}_{\pm\lambda}, which are in the same LL-packet, is the homomorphism

ϕn:WPGL(2,)Gal(/)\phi_{n}\colon W_{\mathbb{R}}\to\operatorname{PGL}(2,\mathbb{C})\rtimes\operatorname{Gal}(\mathbb{C}/\mathbb{R})

defined as follows. Let σGal(/)\sigma\in\operatorname{Gal}(\mathbb{C}/\mathbb{R}) be the nontrivial element, i.e. complex conjugation. For r>0r>0 and θ\theta\in\mathbb{R}, set χn(reiθ)=reinθ\chi_{n}(re^{i\theta})=re^{in\theta}. Then

ϕn(j)=([0(1)n10],σ)ϕn(z)=([χn(z)00χn(z)],e),\begin{split}\phi_{n}(j)&=\Bigl{(}\begin{bmatrix}0&(-1)^{n}\\ 1&0\end{bmatrix},\sigma\Bigr{)}\\ \phi_{n}(z)&=\Bigl{(}\begin{bmatrix}\chi_{n}(z)&0\\ 0&\chi_{-n}(z)\end{bmatrix},e\Bigr{)},\end{split}

for z×z\in\mathbb{C}^{\times}. (See Section I.4 of [Lab].)

2.4 An equivariant index and orbital integrals

Let GG be a connected, real semisimple Lie group with finite centre. Suppose GG acts properly and isometrically on a Riemannian manifold MM. Suppose M/GM/G is compact. Let EME\to M be a 2\mathbb{Z}_{2}-graded, GG-equivariant, Hermitian vector bundle. Let DD be a GG-equivariant, elliptic, self-adjoint first order differential operator on EE that is odd with respect to the grading. The reduced group CC^{*}-algebra CrGC^{*}_{r}G of GG is the closure in the operator norm of the algebra of all convolution operators on L2(G)L^{2}(G) by functions in L1(G)L^{1}(G). Let K0(CrG)K_{0}(C^{*}_{r}G) be its even KK-theory. Then we have the equivariant index of DD

indexG(D)K0(CrG),\operatorname{index}_{G}(D)\in K_{0}(C^{*}_{r}G),

which is the image of the class defined by DD in the equivariant KK-homology group of MM under the analytic assembly map. See [BCH] for details.

Let gGg\in G be a semisimple element, and Z<GZ<G its centraliser. The orbital integral map

fG/Zf(hgh1)d(hZ)f\mapsto\int_{G/Z}f(hgh^{-1})\,d(hZ)

on Cc(G)C_{c}(G), defines a trace map

τg:K0(CrG).\tau_{g}\colon K_{0}(C^{*}_{r}G)\to\mathbb{C}.

See Section 2.1 in [HW2].

Theorem 2.1 in [HW2] is a fixed point formula for the number

τg(indexG(D)).\tau_{g}(\operatorname{index}_{G}(D)).

We will not use this fixed point formula, but only the following localisation or excision property of the index. This property follows directly from Theorem 2.1 in [HW2], but is in fact a step in its proof: see Proposition 4.6 in [HW2].

Proposition 2.10 (Localisation of the index).

Let GG^{\prime}, MM^{\prime}, EE^{\prime} and DD^{\prime} be as GG, MM, EE and DD above, respectively. Suppose that GG and GG^{\prime} are subgroups of some larger group, and that gGGg\in G\cap G^{\prime}. Suppose that there are gg-invariant neighbourhoods UU of the fixed point set MgM^{g} and UU^{\prime} of (M)g(M^{\prime})^{g}, and a diffeomorphism φ:UU\varphi\colon U\to U^{\prime} that commutes with gg, such that

φ(E|U)=E|U,\varphi^{*}(E^{\prime}|_{U^{\prime}})=E|_{U},

and D|UD^{\prime}|_{U^{\prime}} corresponds to D|UD|_{U} under this identification. Then

τg(indexG(D))=τg(indexG(D)).\tau_{g}(\operatorname{index}_{G}(D))=\tau_{g}(\operatorname{index}_{G^{\prime}}(D^{\prime})).

2.5 Discrete series characters as indices

Let K<GK<G be maximal compact. Let T<KT<K be a maximal torus and suppose that TT is a Cartan subgroup of GG; i.e. GG has a discrete series. Let

R:=R(𝔤,𝔱).R:=R(\mathfrak{g}^{\mathbb{C}},\mathfrak{t}^{\mathbb{C}}).

be the root system of (𝔤,𝔱)(\mathfrak{g}^{\mathbb{C}},\mathfrak{t}^{\mathbb{C}}). Choose a positive system R+RR^{+}\subset R, and let ρ\rho be half the sum of the elements of R+R^{+}. Let λi𝔱\lambda\in i\mathfrak{t}^{*} be regular, and dominant with respect to R+R^{+}. Suppose λρ\lambda-\rho is integral. Let πλG\pi^{G}_{\lambda} be the discrete series representation of GG with Harish-Chandra parameter λ\lambda. The values of its character ΘπλG\Theta_{\pi^{G}_{\lambda}} on the regular elements of TT can be realised in terms of index theory.

Consider the GG-manifold G/TG/T, equipped with the GG-invariant Riemannian metric defined by a KK-invariant inner product on 𝔤\mathfrak{g}. Consider the GG-invariant complex structure JR+G/TJ^{G/T}_{R^{+}} on G/TG/T such that, as complex vector spaces,

TeT(G/T)=𝔤/𝔱αR+𝔤α.T_{eT}(G/T)=\mathfrak{g}/\mathfrak{t}\cong\bigoplus_{\alpha\in R^{+}}\mathfrak{g}^{\mathbb{C}}_{\alpha}. (2.4)

Explicitly, this isomorphism is given by the inclusion 𝔤/𝔱(𝔤/𝔱)\mathfrak{g}/\mathfrak{t}\hookrightarrow(\mathfrak{g}/\mathfrak{t})^{\mathbb{C}} followed by projection onto the positive root spaces. Similarly, if wWGw\in W_{G}, then we will write JwR+G/TJ^{G/T}_{wR^{+}} for the complex structure defined as above, with R+R^{+} replaced by wR+wR^{+}.

For any integral element νi𝔱\nu\in i\mathfrak{t}^{*}, we have the GG-equivariant line bundle

LνG:=G×TνG/T.L^{G}_{\nu}:=G\times_{T}\mathbb{C}_{\nu}\to G/T.

Here we write ν\mathbb{C}_{\nu} for the vector space \mathbb{C} on which TT acts with weight ν\nu. Let ¯LλρG\bar{\partial}_{L^{G}_{\lambda-\rho}} be the Dolbeault operator on G/TG/T coupled to LλρGL^{G}_{\lambda-\rho}. Let ¯LλρG\bar{\partial}_{L^{G}_{\lambda-\rho}}^{*} be its formal adjoint with respect to the L2L^{2}-inner product defined by the Riemannian metric on G/TG/T and the natural Hermitian metric on LλρGL^{G}_{\lambda-\rho}.

Proposition 2.11.

If gTregg\in T^{\operatorname{reg}}, then

ΘπλG(g)=(1)dim(G/K)/2τg(indexG(¯LλρG+¯LλρG)).\Theta_{\pi^{G}_{\lambda}}(g)=(-1)^{\dim(G/K)/2}\tau_{g}(\operatorname{index}_{G}(\bar{\partial}_{L^{G}_{\lambda-\rho}}+\bar{\partial}_{L^{G}_{\lambda-\rho}}^{*})).

For a proof, see Propositions 5.1 and 5.2 in [HW2]. This proof is based on the fact that the natural class [πλG]K0(CrG)[\pi_{\lambda}^{G}]\in K_{0}(C^{*}_{r}G) (see e.g.  [Laf]) equals

(1)dim(G/K)/2indexG(¯LλρG+¯LλρG).(-1)^{\dim(G/K)/2}\operatorname{index}_{G}(\bar{\partial}_{L^{G}_{\lambda-\rho}}+\bar{\partial}_{L^{G}_{\lambda-\rho}}^{*}).

3 A geometric proof

Let GG be a connected, real semisimple Lie group with finite centre. Let K<GK<G be a maximal compact subgroup, and suppose a maximal torus T<KT<K is a Cartan subgroup of GG. As before, Let RR be the root system of (𝔤,𝔱)(\mathfrak{g}^{\mathbb{C}},\mathfrak{t}^{\mathbb{C}}), let R+RR^{+}\subset R be a positive system, and let ρ\rho be half the sum of the elements of R+R^{+}. Since GG has a compact Cartan subgroup, it has a compact inner form GcG_{c} by Theorem 2.5. Theorem 2.8 follows from the case where G=GcG^{\prime}=G_{c}, which we will assume from now on. The complexifications 𝔤\mathfrak{g}^{\mathbb{C}} and 𝔤c\mathfrak{g}_{c}^{\mathbb{C}} of the Lie algebras 𝔤\mathfrak{g} and 𝔤c\mathfrak{g}_{c} of GG and GcG_{c}, respectively, are equal. So if we identify TT with a GG_{\mathbb{C}}-conjugate Cartan subgroup Tc<GcT_{c}<G_{c}, then the root system of (𝔤c,𝔱c)(\mathfrak{g}_{c}^{\mathbb{C}},\mathfrak{t}_{c}^{\mathbb{C}}) equals RR. From now on, we will tacitly identify TT and TcT_{c} with each other.

3.1 Identifying open sets

The geometric proof of Theorem 2.8 is based on suitable identifications of neighbourhoods of the fixed point sets of the actions by TT on G/TG/T and Gc/TG_{c}/T.

Let wNGc(T)w\in N_{G_{c}}(T). Consider the TT-invariant complex structure on 𝔤/𝔱\mathfrak{g}/\mathfrak{t} defined by w1R+{w^{-1}R^{+}} and the one on 𝔤c/𝔱\mathfrak{g}_{c}/\mathfrak{t} defined by R+{R^{+}}. Let 𝔱𝔤\mathfrak{t}^{\perp}\subset\mathfrak{g} be the orthogonal complement to 𝔱\mathfrak{t} in 𝔤\mathfrak{g} with respect to an Ad(K)\operatorname{Ad}(K)-invariant inner product. Similarly, let 𝔱c𝔤c\mathfrak{t}^{\perp_{c}}\subset\mathfrak{g}_{c} be the orthogonal complement to 𝔱\mathfrak{t} in 𝔤c\mathfrak{g}_{c}. Then we have a complex-linear isomorphism

ψw:𝔱𝔤/𝔱αR+𝔤w1αAd(w1)αR+𝔤α𝔤c/𝔱𝔱c.\psi_{w}\colon\mathfrak{t}^{\perp}\cong\mathfrak{g}/\mathfrak{t}\cong\bigoplus_{\alpha\in R^{+}}\mathfrak{g}^{\mathbb{C}}_{w^{-1}\alpha}\xrightarrow{\operatorname{Ad}(w^{-1})}\\ \bigoplus_{\alpha\in R^{+}}\mathfrak{g}^{\mathbb{C}}_{\alpha}\cong\mathfrak{g}_{c}/\mathfrak{t}\cong\mathfrak{t}^{\perp_{c}}. (3.1)

Note that Ad(w)\operatorname{Ad}(w) preserves 𝔱c\mathfrak{t}^{\perp_{c}}.

Lemma 3.1.

The composition Ad(w)ψw:𝔱𝔱c\operatorname{Ad}(w)\circ\psi_{w}\colon\mathfrak{t}^{\perp}\to\mathfrak{t}^{\perp_{c}} is TT-equivariant.

Proof.

Let X𝔱X\in\mathfrak{t}^{\perp}. For any choice R~+\tilde{R}^{+} of positive roots, let

pR~+:𝔤/𝔱αR~+𝔤αp_{\tilde{R}^{+}}\colon\mathfrak{g}^{\mathbb{C}}/\mathfrak{t}^{\mathbb{C}}\to\bigoplus_{\alpha\in\tilde{R}^{+}}\mathfrak{g}^{\mathbb{C}}_{\alpha}

be the projection map defined by the root space decomposition. Then

Ad(w)pR+=pw1R+Ad(w).\operatorname{Ad}(w)\circ p_{R^{+}}=p_{w^{-1}R^{+}}\circ\operatorname{Ad}(w).

By definition of ψw\psi_{w},

pR+(ψw(X))=Ad(w1)pw1R+(X).p_{R^{+}}(\psi_{w}(X))=\operatorname{Ad}(w^{-1})p_{w^{-1}R^{+}}(X).

Hence

pw1R+(Ad(w)ψw(X))=Ad(w)pR+(ψw(X))=pw1R+(X).p_{w^{-1}R^{+}}(\operatorname{Ad}(w)\psi_{w}(X))=\operatorname{Ad}(w)p_{R^{+}}(\psi_{w}(X))=p_{w^{-1}R^{+}}(X).

Since pw1R+p_{w^{-1}R^{+}} is TT-equivariant, we have for all hTh\in T,

pw1R+(Ad(h)Ad(w)ψw(X))=pw1R+(Ad(h)X)=pw1R+(Ad(w)ψw(Ad(h)X)).p_{w^{-1}R^{+}}(\operatorname{Ad}(h)\operatorname{Ad}(w)\psi_{w}(X))=p_{w^{-1}R^{+}}(\operatorname{Ad}(h)X)=p_{w^{-1}R^{+}}(\operatorname{Ad}(w)\psi_{w}(\operatorname{Ad}(h)X)).

So Ad(w)ψw\operatorname{Ad}(w)\circ\psi_{w} is indeed TT-equivariant. ∎

The map η:𝔱G/T\eta\colon\mathfrak{t}^{\perp}\to G/T mapping X𝔱X\in\mathfrak{t}^{\perp} to exp(X)T\exp(X)T is TT-equivariant, and a local diffeomorphism near 0𝔱0\in\mathfrak{t}^{\perp}. Let U~𝔱\tilde{U}\subset\mathfrak{t}^{\perp} be an Ad(T)\operatorname{Ad}(T)-invariant open neighbourhood of 0 on which this map defines a diffeomorphism onto its image UG/TU\subset G/T. The tangent map of η\eta at 0 is the identification 𝔱TeTG/T\mathfrak{t}^{\perp}\cong T_{eT}G/T, which is complex-linear by definition. So η(Jw1R+G/T|U)\eta^{*}(J^{G/T}_{w^{-1}R^{+}}|_{U}) is homotopic to Jw1R+|U~J_{w^{-1}R^{+}}|_{\tilde{U}} as TT-invariant complex structures, if we choose U~\tilde{U} small enough. So η\eta is holomorphic up to a homotopy of TT-invariant almost complex structures, which is as good as being holomorphic for index theory purposes.

Let ηc:𝔱cGc/T\eta_{c}\colon\mathfrak{t}^{\perp_{c}}\to G_{c}/T be defined by ηc(Y)=exp(Y)T\eta_{c}(Y)=\exp(Y)T for Y𝔱cY\in\mathfrak{t}^{\perp_{c}}. This is a TT-equivariant map, and a local diffeomorphism near 0. Choose U~\tilde{U} small enough, so that ηc|ψ~w(U~)\eta_{c}|_{\tilde{\psi}_{w}(\tilde{U})} is a diffeomorphism onto its image UcwU_{c}^{w}, which is a neighbourhood of eTeT in Gc/TG_{c}/T. Again, this diffeomorphism is holomorphic up to a TT-equivariant homotopy of complex structures if we choose U~\tilde{U} small enough. For later use, we define the map ηcw:𝔱cGc/T\eta_{c}^{w}\colon\mathfrak{t}^{\perp_{c}}\to G_{c}/T by ηcw(Y)=exp(Y)wT\eta_{c}^{w}(Y)=\exp(Y)wT, for Y𝔱cY\in\mathfrak{t}^{\perp_{c}}. This map is TT-equivariant because ww normalises TT.

The maps ψw\psi_{w}, η\eta and ηc\eta_{c} combine into a diffeomorphism

φw:Uη1U~ψwψw(U)ηcUcw,\varphi_{w}\colon U\xrightarrow{\eta^{-1}}\tilde{U}\xrightarrow{\psi_{w}}\psi_{w}(U)\xrightarrow{\eta_{c}}U_{c}^{w},

holomorphic up to a homotopy of complex structures. The map ψw\psi_{w} is not TT-equivariant, so neither is φw\varphi_{w} in general.

Lemma 3.2.

The composition

wφw:UwUcww\circ\varphi_{w}\colon U\to wU_{c}^{w}

is TT-equivariant.

Proof.

We have

wηc=ηcwAd(w).w\circ\eta_{c}=\eta_{c}^{w}\circ\operatorname{Ad}(w).

Hence

wφw=ηcw(Ad(w)ψw)η1.w\circ\varphi_{w}=\eta_{c}^{w}\circ(\operatorname{Ad}(w)\circ\psi_{w})\circ\eta^{-1}.

The maps ηcw\eta_{c}^{w} and η\eta are TT-equivariant, and by Lemma 3.1, so is Ad(w)ψw\operatorname{Ad}(w)\circ\psi_{w}. So wφww\circ\varphi_{w} is TT-equivariant as well. ∎

3.2 Neighbourhoods of fixed point sets

Let WK:=NK(T)/TW_{K}:=N_{K}(T)/T and WG:=NGc(T)/TW_{G}:=N_{G_{c}}(T)/T. Then WGW_{G} is the Weyl group of the root system RR, which explains the notation WGW_{G}. And WKW_{K} is the subgroup of WGW_{G} generated by reflections defined by compact roots. Note that

(G/T)T=WK(G/T)^{T}=W_{K}

(see Lemma 6.7 in [HW1]), and

(Gc/T)T=WG.(G_{c}/T)^{T}=W_{G}.

Hence we have an inclusion

(G/T)T(Gc/T)T(G/T)^{T}\hookrightarrow(G_{c}/T)^{T}

and

(Gc/T)T=[w]WG/WKw(G/T)T.(G_{c}/T)^{T}=\coprod_{[w]\in W_{G}/W_{K}}w\cdot(G/T)^{T}.

Here we fix representatives wWGw\in W_{G} of all classes [w]WG/WK[w]\in W_{G}/W_{K} once and for all.

Consider the manifold

M:=G/T×WG/WKM:=G/T\times W_{G}/W_{K}

equipped with the action by GG on the first factor. Consider the GG-invariant complex structure on MM such that, for every [w]WG/WK[w]\in W_{G}/W_{K}, the restricted complex structure on G/T×{[w]}G/T\times\{[w]\} is Jw1R+G/TJ^{G/T}_{w^{-1}R^{+}}.

We have TT-invariant neighbourhoods

V:=wKWKwKUV:=\bigcup_{w_{K}\in W_{K}}w_{K}U

of (G/T)T(G/T)^{T} and

Vc:=wWGwUcwV_{c}:=\bigcup_{w\in W_{G}}wU_{c}^{w}

of (Gc/T)T(G_{c}/T)^{T}. We choose the set U~\tilde{U} small enough, the sets wKUw_{K}U and wUcwwU_{c}^{w} are all disjoint, for wKWKw_{K}\in W_{K} and wWGw\in W_{G}. Consider the map

φ:V×WG/WKVc\varphi\colon V\times W_{G}/W_{K}\to V_{c}

given by

φ(wKxT,[w])=wKwφw(xT),\varphi(w_{K}xT,[w])=w_{K}w\varphi_{w}(xT), (3.2)

for wKWKw_{K}\in W_{K}, wWGw\in W_{G} and xTUxT\in U.

Lemma 3.3.

The map φ\varphi is well-defined and TT-equivariant.

Proof.

Let wK,wKNK(T)w_{K},w_{K}^{\prime}\in N_{K}(T) and x,xGx,x^{\prime}\in G be such that wKxT=wKxTw_{K}xT=w_{K}^{\prime}x^{\prime}T. Fix wWGw\in W_{G}. Since the sets wKUw_{K}U and wKUw_{K}^{\prime}U are disjoint if wKw_{K} and wKw_{K}^{\prime} represent different elements of WKW_{K}, there is a tTt\in T such that wK=wKtw_{K}^{\prime}=w_{K}t. There is another tTt^{\prime}\in T such that wKx=wKxtw_{K}^{\prime}x^{\prime}=w_{K}xt^{\prime}. Using TT-equivariance of wφww\varphi_{w} and the fact that wKw_{K} normalises TT, one deduces that wKwφw(xT)=wKwφw(xT)w_{K}^{\prime}w\varphi_{w}(x^{\prime}T)=w_{K}w\varphi_{w}(xT), and that φ\varphi is TT-equivariant. ∎

The arguments in this section lead to the following conclusion.

Proposition 3.4.

The map φ\varphi is a TT-equivariant diffeomorphism, holomorphic up to a homotopy of complex structures, from a TT-invariant neighbourhood of MTM^{T} onto a TT-invariant neighbourhood of (Gc/T)T(G_{c}/T)^{T}.

See Figure 1 for an example of the map φ\varphi.

Remark 3.5.

If one replaces the map φw\varphi_{w} by φe\varphi_{e} in (3.2), one obtains an identification φ~\tilde{\varphi} of neighbourhoods of MTM^{T} and (Gc/T)T(G_{c}/T)^{T} that is simpler than the map φ\varphi we use here. However, φ~\tilde{\varphi} is not TT-equivariant, which is the reason why we use the maps φw\varphi_{w} rather than φe\varphi_{e}. At the same time, using the maps φw\varphi_{w} means that the map φ\varphi is holomorphic up to homotopy with respect to the complex structure on MM described above, whereas the map φ~\tilde{\varphi} is holomorphic up to homotopy if one uses the same complex structure JR+G/TJ^{G/T}_{R^{+}} on all connected components of MM.

3.3 Line bundles

Consider the line bundle LML\to M such that for every [w]WG/WK[w]\in W_{G}/W_{K},

L|G/T×{[w]}=G×Tw1(λρ).L|_{G/T\times\{[w]\}}=G\times_{T}\mathbb{C}_{w^{-1}(\lambda-\rho)}.
Lemma 3.6.

There is a TT-equivariant isomorphism of line bundles

φ(LλρGc|Vc)L|V×WG/WK.\varphi^{*}(L^{G_{c}}_{\lambda-\rho}|_{V_{c}})\cong L|_{V\times W_{G}/W_{K}}.
Lemma 3.7.

Let GG be any Lie group, H<GH<G a compact subgroup, and π:HGL(V)\pi\colon H\to\operatorname{GL}(V) a representation of HH in a finite-dimensional vector space VV. Let xNG(H)x\in N_{G}(H). Consider the representation x1π:HGL(V)x^{-1}\cdot\pi\colon H\to\operatorname{GL}(V) given by (x1π)(h)=π(x1hx)(x^{-1}\cdot\pi)(h)=\pi(x^{-1}hx). Write VπV_{\pi} and Vx1πV_{x^{-1}\cdot\pi} for the vector space VV on which HH acts via π\pi and x1πx^{-1}\cdot\pi, respectively. Fix an Ad(H)\operatorname{Ad}(H)-invariant inner product on 𝔤\mathfrak{g}. Let 𝔥\mathfrak{h}^{\perp} be the orthogonal complement to 𝔥\mathfrak{h} in 𝔤\mathfrak{g}. Define the map ηx:𝔥G/H\eta_{x}\colon\mathfrak{h}^{\perp}\to G/H by ηx(X)=exp(X)xH\eta_{x}(X)=\exp(X)xH, for X𝔥X\in\mathfrak{h}^{\perp}. Let U~𝔥\tilde{U}\subset\mathfrak{h}^{\perp} be an Ad(H)\operatorname{Ad}(H)-invariant open subset such that η|U~\eta|_{\tilde{U}} is a diffeomorphism onto its image UxU_{x}. Then we have an HH-equivariant isomorphism of vector bundles

ηx((G×HVπ)|Ux)U~×Vx1π.\eta_{x}^{*}((G\times_{H}V_{\pi})|_{U_{x}})\cong\tilde{U}\times V_{x^{-1}\cdot\pi}.
Proof.

Note that

ηx((G×HVπ)|Ux)={(X,[exp(X)x,v]);XU~,vVπ}.\eta_{x}^{*}((G\times_{H}V_{\pi})|_{U_{x}})=\{(X,[\exp(X)x,v]);X\in\tilde{U},v\in V_{\pi}\}.

Define the map

f:ηx((G×HVπ)|Ux)U~×Vx1πf\colon\eta_{x}^{*}((G\times_{H}V_{\pi})|_{U_{x}})\to\tilde{U}\times V_{x^{-1}\cdot\pi}

by

f(X,[exp(X)x,v])=(X,v)f(X,[\exp(X)x,v])=(X,v)

for XU~X\in\tilde{U} and vVπv\in V_{\pi}. Note that this map is well-defined, and a vector bundle isomorphism. And for all hHh\in H,

h(X,[exp(X)x,v])=(Ad(h)X,[hexp(X)x,v])=(Ad(h)X,[exp(Ad(h)X)x(x1hx),v])=(Ad(h)X,[exp(Ad(h)X)x,(x1π)(h)v]).\begin{split}h\cdot(X,[\exp(X)x,v])&=(\operatorname{Ad}(h)X,[h\exp(X)x,v])\\ &=(\operatorname{Ad}(h)X,[\exp(\operatorname{Ad}(h)X)x(x^{-1}hx),v])\\ &=(\operatorname{Ad}(h)X,[\exp(\operatorname{Ad}(h)X)x,(x^{-1}\cdot\pi)(h)v]).\end{split}

So

f(h(X,[exp(X)x,v]))=(Ad(h)X,(x1π)(h)v)=hf(X,[exp(X)x,v]).f(h\cdot(X,[\exp(X)x,v]))=(\operatorname{Ad}(h)X,(x^{-1}\cdot\pi)(h)v)=h\cdot f(X,[\exp(X)x,v]).

Proof of Lemma 3.6. Let wNGc(T)w\in N_{G_{c}}(T). The claim is that we have a TT-equivariant isomorphism of line bundles

(wφw)(Gc×Tλρ|wUcw)(G×Tw1(λρ)|U).(w\circ\varphi_{w})^{*}(G_{c}\times_{T}\mathbb{C}_{\lambda-\rho}|_{wU^{w}_{c}})\cong(G\times_{T}\mathbb{C}_{w^{-1}(\lambda-\rho)}|_{U}). (3.3)

By Lemma 3.7, we have isomorphisms of TT-equivariant line bundles

η((G×Tw1(λρ))|U)U~×w1(λρ);(ηcw)((Gc×Tλρ))|wUcw)(ηcw)1(wUcw)×w1(λρ).\begin{split}\eta^{*}((G\times_{T}\mathbb{C}_{w^{-1}(\lambda-\rho}))|_{U})&\cong\tilde{U}\times\mathbb{C}_{w^{-1}(\lambda-\rho)};\\ (\eta_{c}^{w})^{*}((G_{c}\times_{T}\mathbb{C}_{\lambda-\rho}))|_{wU_{c}^{w}})&\cong(\eta_{c}^{w})^{-1}(wU_{c}^{w})\times\mathbb{C}_{w^{-1}(\lambda-\rho)}.\end{split} (3.4)

Now

(ηcw)1(wUcw)=(ηcw)1(wηc(ψw(U~)))=Ad(w)ψw(U~).(\eta_{c}^{w})^{-1}(wU_{c}^{w})=(\eta_{c}^{w})^{-1}(w\eta_{c}(\psi_{w}(\tilde{U})))=\operatorname{Ad}(w)\circ\psi_{w}(\tilde{U}).

By Lemma 3.1, we have a TT-equivariant, holomorphic diffeomorphism

Ad(w)ψw:U~(ηcw)1(wUcw).\operatorname{Ad}(w)\circ\psi_{w}\colon\tilde{U}\xrightarrow{\cong}(\eta_{c}^{w})^{-1}(wU_{c}^{w}).

So the two right hand sides of (3.4) are isomorphic as TT-equivariant line bundles.

We saw in the proof of Lemma 3.2 that

wφwη=ηcw(Ad(w)ψw).w\circ\varphi_{w}\circ\eta=\eta_{c}^{w}\circ(\operatorname{Ad}(w)\circ\psi_{w}).

So the pullback of the left hand side of (3.3) along η\eta equals

(Ad(w)ψw)(ηcw)((Gc×Tλρ))|wUcw)=(Ad(w)ψw)((ηcw)1(wUcw)×w1(λρ))=(ηcwAd(w)ψw)1(wUcw)×w1(λρ).=(wηcψw)1(wUcw)×w1(λρ)=U~×w1(λρ).\begin{split}(\operatorname{Ad}(w)\circ\psi_{w})^{*}(\eta_{c}^{w})^{*}((G_{c}\times_{T}\mathbb{C}_{\lambda-\rho}))|_{wU_{c}^{w}})&=(\operatorname{Ad}(w)\circ\psi_{w})^{*}\bigl{(}(\eta_{c}^{w})^{-1}(wU_{c}^{w})\times\mathbb{C}_{w^{-1}(\lambda-\rho)}\bigr{)}\\ &=(\eta_{c}^{w}\circ\operatorname{Ad}(w)\circ\psi_{w})^{-1}(wU_{c}^{w})\times\mathbb{C}_{w^{-1}(\lambda-\rho)}.\\ &=(w\circ\eta_{c}\circ\psi_{w})^{-1}(wU_{c}^{w})\times\mathbb{C}_{w^{-1}(\lambda-\rho)}\\ &=\tilde{U}\times\mathbb{C}_{w^{-1}(\lambda-\rho)}.\end{split}

The latter line bundle is the pullback of the right hand side of (3.3) along η\eta. \square

3.4 Proof of Theorem 2.8

Since GcG_{c} is compact, the claim is that if ϕ\phi is the LL-parameter of πλG\pi^{G}_{\lambda}, and ϕ\phi^{\prime} is the corresponding LL-parameter for GcG_{c},

(1)dim(G/K)/2πΠϕΘπ|Treg=πΠϕΘπ|Treg.(-1)^{\dim(G/K)/2}\sum_{\pi\in\Pi_{\phi}}\Theta_{\pi}|_{T^{\operatorname{reg}}}=\sum_{\pi^{\prime}\in\Pi_{\phi^{\prime}}}\Theta_{\pi^{\prime}}|_{T^{\operatorname{reg}}}. (3.5)

Let gTg\in T be an element whose powers are dense in TT. Let ¯L\bar{\partial}_{L} be the Dolbeault operator on MM coupled to LL. Propositions 2.10 and 3.4 and Lemma 3.6 imply that

τg(indexGc(¯LλρGc+¯LλρGc))=τg(indexG(¯L+¯L))=[w]WG/WKτg(indexG(¯Lw1(λρ)G+¯Lw1(λρ)G)).\tau_{g}(\operatorname{index}_{G_{c}}(\bar{\partial}_{L^{G_{c}}_{\lambda-\rho}}+\bar{\partial}_{L^{G_{c}}_{\lambda-\rho}}^{*}))=\tau_{g}(\operatorname{index}_{G}(\bar{\partial}_{L}+\bar{\partial}_{L}^{*}))\\ =\sum_{[w]\in W_{G}/W_{K}}\tau_{g}(\operatorname{index}_{G}(\bar{\partial}_{L^{G}_{w^{-1}(\lambda-\rho)}}+\bar{\partial}_{L^{G}_{w^{-1}(\lambda-\rho)}}^{*})). (3.6)

For any regular element νi𝔱\nu\in i\mathfrak{t}^{*}, let ρν\rho_{\nu} be half the sum of the roots in RR with positive inner products with ν\nu. Then for any wWGw\in W_{G}, ρwλ=wρ\rho_{w\lambda}=w\rho. So the right hand side of (3.6) equals

[w]WG/WKτg(index(¯Lw1λρw1λG+¯Lw1λρw1λG)).\sum_{[w]\in W_{G}/W_{K}}\tau_{g}(\operatorname{index}(\bar{\partial}_{L^{G}_{w^{-1}\lambda-\rho_{w^{-1}\lambda}}}+\bar{\partial}_{L^{G}_{w^{-1}\lambda-\rho_{w^{-1}\lambda}}}^{*})).

By Proposition 2.11, this equals

(1)dim(G/K)/2[w]WG/WKΘπw1λG(g).(-1)^{\dim(G/K)/2}\sum_{[w]\in W_{G}/W_{K}}\Theta_{\pi^{G}_{w^{-1}\lambda}}(g).

As noted below Proposition 2.7, we have

Πϕ={πwλG;wWG}/WK,\Pi_{\phi}=\{\pi^{G}_{w\lambda};w\in W_{G}\}/W_{K},

and similarly,

Πϕ={πλGc}.\Pi_{\phi^{\prime}}=\{\pi^{G_{c}}_{\lambda}\}.

Note that πλGc\pi^{G_{c}}_{\lambda} is the irreducible representation of GcG_{c} with infinitesimal character λ\lambda, so with highest weight λρ\lambda-\rho. The Borel–Weil–Bott theorem therefore implies that the right hand side of (3.5), evaluated at gg, equals

ΘπλGc(g)=τg(indexGc(¯LλρGc+¯LλρGc)),\Theta_{\pi^{G_{c}}_{\lambda}}(g)=\tau_{g}(\operatorname{index}_{G_{c}}(\bar{\partial}_{L^{G_{c}}_{\lambda-\rho}}+\bar{\partial}_{L^{G_{c}}_{\lambda-\rho}}^{*})),

which by the above considerations equals the left hand side of (3.5), evaluated at gg. We have assumed that the powers of gg are dense in TT, but as such elements are dense in TregT^{\operatorname{reg}}, Theorem 2.8 follows in the case where G=GcG^{\prime}=G_{c} since both sides of (3.5) are analytic on TregT^{\operatorname{reg}}. As noted at the start of Section 3, that case implies the general case, so the theorem has been proved.

3.5 Example: G=SL(2,)G=\operatorname{SL}(2,\mathbb{R})

Let G=SL(2,)G=\operatorname{SL}(2,\mathbb{R}), and G=Gc=SU(2)G^{\prime}=G_{c}=\operatorname{SU}(2). Note that GG is quasi-split. Take K=T=SO(2)U(1)SU(2)K=T=\operatorname{SO}(2)\cong\operatorname{U}(1)\hookrightarrow\operatorname{SU}(2). Let ρi𝔱\rho\in i\mathfrak{t}^{*} be the element mapping X:=[0110]𝔱X:=\begin{bmatrix}{0}&{-1}\\ {1}&{0}\end{bmatrix}\in\mathfrak{t} to ii. Let nn\in\mathbb{N}, and set λ=nρ\lambda=n\rho. Let π±λG\pi^{G}_{\pm\lambda} be the discrete series representation of SL(2,)\operatorname{SL}(2,\mathbb{R}) with Harish-Chandra parameter ±λ\pm\lambda. Let ϕ\phi be the LL-parameter of πλG\pi^{G}_{\lambda}; see Example 2.9. Then Πϕ={πλG,πλG}\Pi_{\phi}=\{\pi^{G}_{\lambda},\pi^{G}_{-\lambda}\}. Let ϕ\phi^{\prime} be the corresponding LL-parameter for GcG_{c}. Then Πϕ={πλGc}\Pi_{\phi^{\prime}}=\{\pi^{G_{c}}_{\lambda}\}, where πλGc\pi^{G_{c}}_{\lambda} is the irreducible representation of SU(2)\operatorname{SU}(2) with infinitesimal character λ\lambda, so with highest weight λρ\lambda-\rho.

Fix gTg\in T with dense powers. Now Gc/T=S2G_{c}/T=S^{2}, and (Gc/T)g(G_{c}/T)^{g} consists of the north and south poles. And G/TG/T is the hyperbolic plane {x2+y2z2=n}\{x^{2}+y^{2}-z^{2}=n\}, and (G/T)g(G/T)^{g} is the single point eT=(0,0,n)eT=(0,0,n). We have WK={e}W_{K}=\{e\} and WG=2W_{G}=\mathbb{Z}_{2}, where the nontrivial element of WGW_{G} is represented by333Note that as matrices, we have w=Xw=X. We use different letters because ww is viewed as a group element, whereas XX is viewed as a Lie algebra element. w:=[0110]NSU(2)(U(1))w:=\begin{bmatrix}{0}&{-1}\\ {1}&{0}\end{bmatrix}\in N_{\operatorname{SU}(2)}(\operatorname{U}(1)). This element maps the north pole of Gc/T=S2G_{c}/T=S^{2} to the south pole. So we see that indeed

(Gc/T)g=(G/T)gw(G/T)g,(G_{c}/T)^{g}=(G/T)^{g}\cup w(G/T)^{g},

The map φ\varphi identifying neighbourhoods of these fixed point sets in Gc/TG_{c}/T and G/T×WG/WKG/T\times W_{G}/W_{K}, respectively, is depicted in Figure 1.

The Atiyah–Segal–Singer or Atiyah–Bott fixed point formula implies that, if g=exp(tX)g=\exp(tX),

indexSU(2)(¯LλρSU(2)+¯LλρSU(2))(g)=eλ(g)eλ(g)eρ(g)eρ(g)=sin(nt)sin(t).\operatorname{index}_{\operatorname{SU}(2)}(\bar{\partial}_{L^{\operatorname{SU}(2)}_{\lambda-\rho}}+\bar{\partial}_{L^{\operatorname{SU}(2)}_{\lambda-\rho}}^{*})(g)=\frac{e^{\lambda}(g)-e^{-\lambda}(g)}{e^{\rho}(g)-e^{-\rho}(g)}=\frac{\sin(nt)}{\sin(t)}. (3.7)

Theorem 2.1 in [HW2] implies that

τg(indexSL(2,)(¯L±(λρ)SL(2,)+¯L±(λρ)SL(2,)))=e±λ(g)±(eρ(g)eρ(g))=±e±int2isin(t).\tau_{g}(\operatorname{index}_{\operatorname{SL}(2,\mathbb{R})}(\bar{\partial}_{L^{\operatorname{SL}(2,\mathbb{R})}_{\pm(\lambda-\rho)}}+\bar{\partial}_{L^{\operatorname{SL}(2,\mathbb{R})}_{\pm(\lambda-\rho)}}^{*}))=\frac{e^{\pm\lambda}(g)}{\pm(e^{\rho}(g)-e^{-\rho}(g))}=\pm\frac{e^{\pm int}}{2i\sin(t)}.

Let ϕ\phi be the LL-parameter of πλG\pi^{G}_{\lambda}, and let ϕ\phi^{\prime} be the corresponding LL-parameter for SU(2)\operatorname{SU}(2). Then we conclude that

(1)dim(SL(2,)/SO(2))/2πΠϕΘπ(g)=τg(indexSL(2,)(¯LλρSL(2,)+¯LλρSL(2,)))+τg(indexSL(2,)(¯L(λρ)SL(2,)+¯L(λρ)SL(2,)))=indexSU(2)(¯LλρSU(2)+¯LλρSU(2))(g)=(1)dim(SU(2)/SU(2))/2πΠϕΘπ(g).(-1)^{\dim(\operatorname{SL}(2,\mathbb{R})/\operatorname{SO}(2))/2}\sum_{\pi\in\Pi_{\phi}}\Theta_{\pi}(g)=\\ \tau_{g}(\operatorname{index}_{\operatorname{SL}(2,\mathbb{R})}(\bar{\partial}_{L^{\operatorname{SL}(2,\mathbb{R})}_{\lambda-\rho}}+\bar{\partial}_{L^{\operatorname{SL}(2,\mathbb{R})}_{\lambda-\rho}}^{*}))+\tau_{g}(\operatorname{index}_{\operatorname{SL}(2,\mathbb{R})}(\bar{\partial}_{L^{\operatorname{SL}(2,\mathbb{R})}_{-(\lambda-\rho)}}+\bar{\partial}_{L^{\operatorname{SL}(2,\mathbb{R})}_{-(\lambda-\rho)}}^{*}))=\\ \operatorname{index}_{\operatorname{SU}(2)}(\bar{\partial}_{L^{\operatorname{SU}(2)}_{\lambda-\rho}}+\bar{\partial}_{L^{\operatorname{SU}(2)}_{\lambda-\rho}}^{*})(g)=\\ (-1)^{\dim(\operatorname{SU}(2)/\operatorname{SU}(2))/2}\sum_{\pi^{\prime}\in\Pi_{\phi^{\prime}}}\Theta_{\pi^{\prime}}(g).

In this example, we see from the fixed point formulas used, and Weyl’s and Harish-Chandra’s character formulas, that the respective indices evaluated at gg equal the characters of the corresponding representations. And the character identity follows directly from the explicit expressions for these characters. But note that in the proof of Theorem 2.8, these fixed point formulas and character formulas were not used.

Refer to caption
Figure 1: The map φ\varphi for G=SL(2,)G=\operatorname{SL}(2,\mathbb{R})

References

  • [ABV] J. Adams, D. Barbasch, D.A. Vogan Jr., The Langlands classification and irreducible characters for real reductive groups. Progress in Mathematics, v. 104, Birkhäuser Boston, Inc., Boston, MA, 1992. xii+318 pp.
  • [A] J. Arthur, An introduction to the trace formula. Clay Mathematics Proceedings, Vol 4, 2005.
  • [AS2] M.F. Atiyah, G.B. Segal, The index of elliptic operators. II. Ann. of Math. (2) 87, 531€–545, 1968.
  • [AS1] M.F. Atiyah, I.M. Singer, The index of elliptic operators. I. Ann. of Math. (2) 87, 484–530, 1968.
  • [BCH] P. Baum, Alain Connes, and Nigel Higson. Classifying space for proper actions and K-theory of group CC^{*}-algebras. In CC^{*}-algebras: 1943–1993 (San Antonio, TX, 1993), volume 167 of Contemp. Math., pages 240–291. American Mathematical Society, Providence, RI, 1994.
  • [B] A. Borel, Linear algebraic groups. Modern Birkhäuser Classics, Springer, T.A., Reprint of 1998 2nd edition.
  • [HC1] Harish-Chandra, Discrete series for semisimple Lie groups. I. Construction of invariant eigendistributions. Acta Math. 113, 241–318, 1965.
  • [HC2] Harish-Chandra, Discrete series for semisimple Lie groups. II. Explicit determination of the characters. Acta Math., 116:1–111, 1966.
  • [HW1] P. Hochs, H. Wang, A fixed point theorem on noncompact manifolds. Annals of K-theory (to appear).
  • [HW2] P. Hochs, H. Wang, A fixed point theorem and Harish-Chandra character formula. Proceedings of the London Mathematical Society (3) 00, 1–32, 2017.
  • [Kn1] A.W. Knapp, Representation theory of semisimple groups, Princeton University Press, 1986.
  • [Lab] J.-P. Labesse, Introduction to endoscopy, Representation Theory of real reductive Lie groups, Contemporary Mathematics, 472, AMS, 175–213, 2008.
  • [Laf] V. Lafforgue, Banach KKKK-theory and the Baum-Connes conjecture. In Proceedings of the International Congress of Mathematicians, Vol. II (Beijing, 2002), pages 795–812. Higher Ed. Press, Beijing, 2002.
  • [L1] R.P. Langlands, Letter to Prof. Weil, 1967.
  • [L2] R.P. Langlands, Problems in the theory of automorphic forms, Lectures in modern analysis and applications, III, Lecture Notes in Math 170, Springer-Verlag, pp. 18–61, 1970.
  • [L3] R.P. Langlands, On the classification of irreducible representations of real algebraic groups, Representation Theory and Harmonic Analysis on Semisimple Lie Groups, Mathematical Surveys and Monographs, No.13, AMS, 101–170, 1989.
  • [S1] D. Shelstad, Some character relations for real reductive algebraic groups, Thesis (Ph.D.), Yale University, 59 pp, 1974.
  • [S2] D. Shelstad, Character and inner forms of a quasi-split group over \mathbb{R}, Compositio Mathematica, Vol. 39, Fasc. 1, 11–45, 1979.
  • [T] J. Throne, Topics in automorphic forms. Online lecture notes www.math.harvard.edu/~jbland/ma270x_notes.pdf, 2013.