Bourbaki

§ 7. Irreducible representations of connected compact Lie groups

We retain the notations of §6. A representation of G is a continuous (hence analytic) homomorphism from G to a group GL(V)\mathbf{G}\mathbf{L}(V), where V is a finite dimensional complex vector space. Every representation of G is semi-simple (§1, no. 1).

Choose a chamber C of t(\mathfrak{t}(§5, no. 2), and put Γ(T)++=C‾∩Γ(T)\Gamma (T)_{++}=\overline{C}\cap \Gamma (T).

1. Dominant characters

Denote by X+X_+ the set of elements λ\lambda of X(T) such that ⟨λ,x⟩≥0\langle \lambda , x\rangle \geq 0 for all x∈Γ(T)++x\in \Gamma (T)_{++}, that is, such that the linear form δ(λ):tC→C\delta (\lambda ) :\mathfrak{t}_{\mathbf{C}}\rightarrow \mathbf{C} maps the chamber C of t\mathfrak{t} to iR+i\mathbf{R}_+.

Give X(T) the ordered group structure for which the positive elements are those of X+X_+; put R+=R(G,T)∩X+R_+= R(G,T)\cap X_+ and R−=−R+R_-=-R_+. The elements of R+R_+ are called positive roots, those of R−R_- negative roots; every root is either positive or negative (Chap. VI, §1, no. 6, Th. 3). A positive root that is not the sum of two positive roots is said to be simple; every positive root is a sum of simple roots (loc. cit.); the simple roots form a basis of the subgroup of X(T) generated by the roots, a subgroup that can be identified with X(T/C(G))X(T/C(G)) (§4, no. 4); the reflections with respect to the simple roots generate the Weyl group W=WG(T)W = W_G(T) (Chap. VI, §1, no. 5, Th. 2).

Lemma 1 01FZ

Let λ\lambda be an element of X(T). The following conditions are equivalent:

(i) λ−w(λ)≥0\lambda -w(\lambda )\geq 0 (resp. >0>0) for all w∈Ww\in W such that w≠1w\not= 1;

(ii) for all w∈Ww\in W such that w≠1,λ−w(λ)w\not= 1,\lambda -w(\lambda ) is a linear combination with positive coefficients (resp. positive coefficients not all zero) of simple roots;

(iii) ⟨λ,Kα⟩≥0\langle \lambda , K_{\alpha}\rangle \geq 0 (resp. >0>0) for every positive root α\alpha;

(iv) ⟨λ,Kα⟩≥0\langle \lambda , K_{\alpha}\rangle \geq 0 (resp. >0>0) for every simple root α\alpha.

The equivalence if (iii) and (iv) is immediate. Since the set of the KαK_{\alpha} can be identified with the inverse root system of R(G,T)(R(G,T) (§4, no. 5), the equivalence of (i) and (iii) follows from Chap. VI, §1, no. 6, Prop. 18 and Cor. The implication (ii) ⇒\Rightarrow (i) is trivial, and the opposite implication follows from loc. cit.

Denote by X++X_{++} the set of elements of X(T) such that ⟨λ,Kα⟩≥0\langle \lambda , K_{\alpha}\rangle \geq 0 for every positive root α\alpha. The elements of X++X_{++} are said to be dominant. They form a fundamental domain for the operation of W on X(T) (Chap. VI, §1, no. 10). We have X++⊂X+X_{++}\subset X_+.

If G is simply-connected, for each simple root α\alpha there exists an element ϖα\varpi_{\alpha} of X(T) such that ⟨ϖβ,Kα⟩=δαβ\langle \varpi_{\beta}, K_{\alpha}\rangle =\delta_{\alpha \beta} for every simple root β\beta, that is, sα(ϖα)=s_{\alpha}(\varpi_{\alpha}) = ϖα−α,sβ(ϖα)=ϖα\varpi_{\alpha}-\alpha ,s_{\beta}(\varpi_{\alpha}) =\varpi_{\alpha} for every simple root β≠α\beta \not=\alpha; the ϖα\varpi_{\alpha} are called the fundamental dominant weights; they form a basis of the commutative group X(T) and of the commutative monoid X++X_{++}; more precisely, every element λ\lambda of X(T) can be written in the form λ=∑α⟨λ,Kα⟩ϖα\lambda =\sum_{\alpha}\langle \lambda , K_{\alpha}\rangle \varpi_{\alpha}.

Denote by ρ\rho the element of X(T)⊗QX(T)\otimes \mathbf{Q} such that

2ρ=∑α∈R+α 2\rho =\sum_{\alpha\in R_+}\alpha

We have ⟨ρ,Kα⟩=1\langle \rho , K_{\alpha}\rangle = 1 for every simple root α\alpha (Chap. VI, §1, no. 10, Prop. 29). If G is simply-connected, ρ\rho is the sum of the fundamental dominant weights.

2. Highest weight of an irreducible representation

Associate to any representation τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) the homomorphism L(τ)(C)L(\tau )_{(\mathbf{C})} from the C\mathbf{C}-Lie algebra gC\mathfrak{g}_{\mathbf{C}} to End(V) extending the linear representation L(τ)L(\tau ) of g\mathfrak{g} on the real vector space underlying V (Chap. III, §3, no. 11). By Prop. 7 of §4, no. 3, the map δ\delta from X(T) to HomC(tC,C)=tC∗_{\mathbf{C}}(\mathfrak{t}_{\mathbf{C}},\mathbf{C}) =\mathfrak{t}^*_{\mathbf{C}} induces a bijection from the set of weights of τ\tau relative to T to the set of weights of L(τ)(C)L(\tau )_{(\mathbf{C})} relative to the Cartan subalgebra tC\mathfrak{t}_{\mathbf{C}} of gC\mathfrak{g}_{\mathbf{C}}.

Lemma 2 01G0

Let φ\varphi be a linear representation of the complex Lie algebra gC\mathfrak{g}_{\mathbf{C}} on a finite dimensional complex vector space V. There exists a representation τ\tau of G on V such that L(τ)(C)=φL(\tau )_{(\mathbf{C})}=\varphi if and only if φ\varphi is semi-simple and the weights of tC\mathfrak{t}_{\mathbf{C}} on V belong to δ(X(T))\delta (X(T)).

If there exists a representation τ\tau of G such that L(τ)(C)=φL(\tau )_{(\mathbf{C})}=\varphi, then φ\varphi is semi-simple because G is connected and τ\tau is semi-simple (Chap. III, §6, no. 5, Cor. 2 of Prop. 13), and the weights of tC\mathfrak{t}_{\mathbf{C}} on V belong to the image of δ\delta. Thus, the condition is necessary; we shall prove that it is sufficient. If φ\varphi is semi-simple, V is the direct sum of the Vμ(tC)V_\mu(\mathfrak{t}_{\mathbf{C}}), where μ\mu belongs to the set of weights of tC\mathfrak{t}_{\mathbf{C}} on V (Chap. VII, §2, no. 4, Cor. 3 of Th. 2); if all the weights belong to the image of δ\delta, there exists a representation τT\tau_T of T on V such that L(τT)(C)=φ∣tC:L(\tau_T)_{(\mathbf{C})}=\varphi |\mathfrak{t}_{\mathbf{C}}: indeed, it suffices to put τT(t)v=tλv\tau_T(t)v=t^{\lambda}v for t∈Tt\in T and v∈Vδ(λ)(tC)v\in V_{\delta(\lambda)}(\mathfrak{t}_{\mathbf{C}}). The lemma now follows from Prop. 8 of §2, no. 6.

Theorem 1 01G1

a) Let τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) be an irreducible representation of G. Then the set of weights of τ\tau (relative to T) has a largest element λ\lambda, which is dominant, and the space Vλ(T)V_{\lambda}(T) is of dimension 1.

b) Two irreducible representations of G are equivalent if and only if their highest weights are equal.

c) For every dominant element λ\lambda of X(T), there exists an irreducible representation of G of highest weight λ\lambda.

By Lemma 2, the equivalence classes of irreducible representations of G correspond bijectively to the classes of finite dimensional irreducible representations of g\mathfrak{g} whose weights belong to δ(X(T))\delta (X(T)).

Denote by CgC\mathscr{C}\mathfrak{g}_{\mathbf{C}} the centre and by DgC\mathscr{D}\mathfrak{g}_{\mathbf{C}} the derived Lie algebra of gC\mathfrak{g}_{\mathbf{C}}, so that gC=CgC⊕DgC\mathfrak{g}_{\mathbf{C}}=\mathscr{C}\mathfrak{g}_{\mathbf{C}}\oplus \mathscr{D}\mathfrak{g}_{\mathbf{C}}. For every bilinear form μ\mu on tC∩DgC\mathfrak{t}_{\mathbf{C}}\cap \mathscr{D}\mathfrak{g}_{\mathbf{C}}, denote by E(μ)E(\mu) the simple DgC\mathscr{D}\mathfrak{g}_{\mathbf{C}}-module introduced in Chap. VIII, §6, no. 3; for every linear form ν\nu on CgC\mathscr{C}\mathfrak{g}_{\mathbf{C}}, denote by C(ν)\mathbf{C}(\nu ) the 1-dimensional CgC\mathscr{C}\mathfrak{g}_{\mathbf{C}}-module over C\mathbf{C} associated to it. Then the gC\mathfrak{g}_{\mathbf{C}}-modules C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu) are simple, and by Chap. VIII, §7, no. 2, Cor. 2 of Th. 1 and Algebra, Chap. VIII, §11, no. 1, Th. 1, every finite dimensional simple gC\mathfrak{g}_{\mathbf{C}}-module is isomorphic to one of the modules C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu); moreover (loc. cit.)C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu) is finite dimensional if and only if μ(Hα)\mu(H_{\alpha}) is a positive integer for every simple root α\alpha. If we denote by ν+μ\nu +\mu the linear form on tC\mathfrak{t}_{\mathbf{C}} that induces ν\nu on CgC\mathscr{C}\mathfrak{g}_{\mathbf{C}} and μ\mu on tC∩DgC\mathfrak{t}_{\mathbf{C}}\cap \mathscr{D}\mathfrak{g}_{\mathbf{C}}, then (ν+μ)(Hα)=μ(Hα)(\nu +\mu)(H_{\alpha}) =\mu(H_{\alpha}); moreover, the weights of C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu) are the ν+λ\nu +\lambda, where λ\lambda is any weight of E(μ)E(\mu), and are thus of the form ν+μ−θ\nu +\mu-\theta, with θ∈δ(X+)\theta \in \delta (X_+) (Chap. VIII, §6, no. 2, Lemma 2).

We conclude that the g\mathfrak{g}-module C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu) is finite dimensional if and only if (ν+μ)(Hα)(\nu +\mu)(H_{\alpha}) is a positive integer for every simple root α\alpha, and that its weights belong to δ(X(T))\delta (X(T)) if and only if ν+μ\nu +\mu belongs to δ(X(T))\delta (X(T)). The conjunction of these two conditions means that ν+μ\nu +\mu belongs to δ(X++)\delta (X_{++}); in that case, ν+μ\nu +\mu is the highest weight of C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu). Thus, we have constructed for every dominant weight λ\lambda of X(T) an irreducible representation of G of highest weight λ\lambda, and have thus obtained, up to equivalence, all the irreducible representations of G. Since the vectors of weight ν+μ\nu +\mu in C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu) form a subspace of dimension 1, the proof is complete.

Corollary 01G2

The group G has a (finite dimensional) faithful linear representation.

Observe first that every element of X(T) is equal to the difference of two dominant weights: more precisely, let ϖ\varpi be an element of X++X_{++} such that ⟨ϖ,Kα⟩>0\langle \varpi , K_{\alpha}\rangle >0 for every simple root α\alpha; for all λ∈X(T)\lambda \in X(T) there exists a positive integer nn such that ⟨λ+nϖ,Kα⟩≥0\langle \lambda +n\varpi , K_{\alpha}\rangle \geq 0 for every simple root α\alpha, that is (no. 1, Lemma 11)λ+nϖ∈X++\lambda +n\varpi \in X_{++}.

Consequently, there exists a finite family (λi)i∈I(\lambda_i)_{i\in I} of elements of X++X_{++} generating the Z\mathbf{Z}-module X(T). For i∈Ii\in I, let τi\tau_i be an irreducible representation of G of highest weight λi\lambda_i (Th. 1); let the representation τ\tau be the direct sum of the τi\tau_i. By construction the set P(τ,T)P(\tau ,T) of weights of τ\tau (relative to T) generates the Z\mathbf{Z}-module X(T). It now follows from Prop. 6 of §4, no. 3 that the homomorphism τ\tau is injective, hence the corollary.

Remark 1 01G3

Let n+\mathfrak{n}_+ be the subalgebra of gC\mathfrak{g}_{\mathbf{C}} that is the sum of the gα\mathfrak{g}^{\alpha} for α>0\alpha >0. Let τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) be an irreducible representation, λ∈X++\lambda \in X_{++} its highest weight and τ′:gC→gl(V)\tau ':\mathfrak{g}_{\mathbf{C}}\rightarrow \mathfrak{g}\mathfrak{l}(V) the representation induced by τ\tau. Then Vλ(T)V_{\lambda}(T) is the subspace consisting of the vectors vv in V such that τ′(x)v=0\tau '(x)v= 0 for all x∈n+x\in \mathfrak{n}_+.

Indeed, this follows from the corresponding statement for the gC\mathfrak{g}_{\mathbf{C}}-modules C(ν)⊗E(μ)\mathbf{C}(\nu )\otimes E(\mu) (Chap. VIII, §6, no. 2, Prop. 3).

Remark 2 01G4

Let Θ(G)\Theta (G) be the algebra of continuous representative functions on G with values in C(\mathbf{C}(Algebra, Chap. VIII). Let G operate on Θ(G)\Theta (G) by left and right translations. For each λ∈X++\lambda \in X_{++}, let (Vλ,τλ)(V_{\lambda}, \tau_{\lambda}) be an irreducible representation of G of highest weight λ\lambda (Th. 1), and (Vλ∗,τˇλ)(V^*_{\lambda},\check{\tau}_{\lambda}) the contragredient representation (Chap. III, §3, no. 11); by Spectral Theories, the representation of G×GG\times G on Θ(G)\Theta (G) is isomorphic to the direct sum of the representations (Vλ⊗Vλ∗,τλ⊗τˇλ)(V_{\lambda}\otimes V^*_{\lambda}, \tau_{\lambda}\otimes \check{\tau}_{\lambda}) for all λ\lambda in X++X_{++}. Remark 1 now implies the following statement: Let λ∈X++\lambda \in X_{++}, and let EλE_{\lambda} be the vector subspace of Θ(G)\Theta (G) consisting of the continuous representative functions ff on G such that f(gt)=λ(t)−1f(g)f(gt) =\lambda (t)^{-1}f(g) for all g∈Gg\in G and all t∈Tt\in T, and such that f∗x=0f*x= 0 for all x∈n−=⨁α<0gαx\in \mathfrak{n}_-=\bigoplus_{\alpha <0}\mathfrak{g}^{\alpha}.

Then EλE_{\lambda} is stable under left translations, and the representation of G on EλE_{\lambda} by left translations is irreducible of highest weight λ\lambda.

Remark 3 01G5

Let τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) be an irreducible representation. There exists an element ν\nu of X(C(G)) such that τ(s)v=ν(s)v\tau (s)v=\nu (s)v for all s∈C(G),v∈V:s\in C(G), v\in V: indeed, τ(C(G))\tau (C(G)) is contained in the commutant of τ\tau(G), which is equal to C∗.1V(\mathbf{C}^*.1_V(Algebra, Chap. VIII, §3, no. 2, Th. 1). For every weight λ\lambda of τ\tau, the restriction of λ\lambda to C(G) is equal to ν\nu.

Remark 4 01G6

The definitions and statements of Chap. VIII, §7, nos. 2 to 5 can be generalized without difficulty to the present situation; we leave the details to the reader.

Proposition 1 01G7

Let τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) be an irreducible representation of G of highest weight λ∈X++\lambda \in X_{++}. Let mm be the integer ∑α∈R+⟨λ,Kα⟩\sum_{\alpha\in R_+}\langle \lambda , K_{\alpha}\rangle, and let w0w_0

be the element of the Weyl group such that w0(R+)=R−w_0(R_+) = R_- (Chap. VI, § 6, Cor. 3 of Prop. 17). There are three possible cases:

a)w0(λ)=−λ)w_0(\lambda ) =-\lambda and mm is even. Then there exists a G-invariant separating symmetric bilinear form on V; the representation τ\tau is of real type (Appendix II).

b)w0(λ)≠−λ)w_0(\lambda )\not=-\lambda. Every G-invariant bilinear form on V is zero; the representation τ\tau is of complex type (loc. cit.).

c)w0(λ)=−λ)w_0(\lambda ) =-\lambda and mm is odd. Then there exists a G-invariant separating alternating bilinear form on V; the representation τ\tau is of quaternionic type (loc. cit.).

If the restriction of τ\tau to C(G)0C(G)_0 is not trivial, we are in case b).

A bilinear form B on V is invariant under G if and only if it is invariant under gC\mathfrak{g}_{\mathbf{C}} (Chap. III, §6, no. 5, Cor. 3). Thus, if G is semi-simple, the proposition follows from Chap. VIII, §7, no. 5, Prop. 12 and Prop. 3 of Appendix II.

In the general case, put C(G)0=SC(G)_0= S, and identify X(T/S)X(T/S) with a subgroup of X(T) (stable under W). If τ(S)={1V},τ\tau (S) =\{1_V\},\tau induces by passage to the quotient a representation τ′:G/S→GL(V)\tau ': G/S\rightarrow \mathbf{G}\mathbf{L}(V) of highest weight λ\lambda; in this case the proposition follows from the preceding, applied to G/SG/S.

Assume that τ(S)≠{1V}\tau (S)\not=\{1_V\}. There exists a non-zero element ν\nu of X(S) such that τ(s)=ν(s)V\tau (s) =\nu (s)_V for all s∈Ss\in S (Remark 3). Then ν\nu is the image of λ\lambda under the restriction homomorphism X(T)→X(S)X(T)\rightarrow X(S); since W operates trivially on X(S), the equality w0(λ)=−λw_0(\lambda ) =-\lambda implies that ν=−ν\nu =-\nu, which is impossible: hence w0(λ)≠−λw_0(\lambda )\not=-\lambda. On the other hand, if B is a G-invariant bilinear form on V, we have, for all x,yx, y in V and ss in S,

B(ν(s)x,ν(s)y)=B(x,y)=ν(s)2B(x,y) B(\nu (s)x, \nu (s)y) = B(x, y) =\nu (s)^2B(x, y)

which implies that B = 0, hence the proposition.

Let SR(G)\mathfrak{S}_{\mathbf{R}}(G) be the set of classes of irreducible continuous representations of G on finite dimensional real vector spaces. Prop. 1 and the results of Appendix II give a bijection Φ:X++/Σ→SR\Phi : X_{++}/\Sigma \rightarrow \mathfrak{S}_{\mathbf{R}}(G), where Σ\Sigma denotes the subgroup {1,−w0}\{1,-w_0\} of Aut(X(T)). More precisely, let λ∈X++\lambda \in X_{++}, and let EλE_{\lambda} be a representation of G of highest weight λ\lambda; then

Φ({λ,−w0(λ)})=Eλ[R]\Phi (\{\lambda ,-w_0(\lambda )\}) = E_{\lambda[\mathbf{R}]} if λ≠−w0(λ)\lambda \not=-w_0(\lambda ) or if ∑α∈R+⟨λ,Kα⟩∉2Z\sum_{\alpha\in R_+}\langle \lambda , K_{\alpha}\rangle \notin2\mathbf{Z}

Φ({λ,−w0(λ)})=Eλ′\Phi (\{\lambda ,-w_0(\lambda )\}) = E'_{\lambda} if λ=−w0(λ)\lambda =-w_0(\lambda ) and ∑α∈R+⟨λ,Kα⟩∈2Z\sum_{\alpha\in R_+}\langle \lambda , K_{\alpha}\rangle \in 2\mathbf{Z}

where Eλ′E'_{\lambda} is an R\mathbf{R}-structure on EλE_{\lambda} invariant under G.

3. The ring r(g)

Let R(G) be the ring of representations (continuous, on finite dimensional complex vector spaces) of G (Algebra, Chap. VIII, §10, no. 6). If τ\tau is a representation of G, denote by [τ][\tau ] its class in R(G); if τ\tau and τ′\tau ' are two representations of G, we have, by definition,

[τ]+[τ′]=[τ⊕τ′] [\tau ] + [\tau '] = [\tau \oplus \tau ']
[τ][τ′]=[τ⊗τ′] [\tau ][\tau '] = [\tau \otimes \tau ']

Since every representation of G is semi-simple, the Z\mathbf{Z}-module R(G) is free and admits as a basis the set of classes of irreducible representations of G, a set that can be identified with X++X_{++} by Th. 1. The map τ→L(τ)(C)\tau \rightarrow L(\tau )_{(\mathbf{C})} induces a homomorphism ll from the ring R(G) to the ring R(gC)\mathscr{R}(\mathfrak{g}_{\mathbf{C}}) of representations of gC\mathfrak{g}_{\mathbf{C}} (Chap. VIII, §7, no. 6).

Let τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) be a representation of G; we consider the gradation (Vλ(T))λ∈X(T)(V_{\lambda}(T))_{\lambda\in X(T)} of the C\mathbf{C}-vector space V. Denote by Ch(V), or by Ch(τ\tau ), the character of the graded vector space V (Chap. VIII, §7, no. 7); if (eλ)λ∈X(T)(e^{\lambda})_{\lambda\in X(T)} denotes the canonical basis of the algebra Z[X(T)]=Z(X(T))\mathbf{Z}[X(T)] =\mathbf{Z}^{(X(T))}, we have, by definition,

Ch(τ\tau ) =∑λ∈X(T)=\sum_{\lambda\in X(T)}(dim Vλ(T)V_{\lambda}(T))eλe^{\lambda}.

We define in the same way (loc. cit.) a homomorphism of rings, also denoted by Ch, from R(G) to Z[X(T)]\mathbf{Z}[X(T)]. If G is semi-simple, we have a commutative diagram

R(G) ⟶ChZ[X(T)]\longrightarrow^{Ch}\mathbf{Z}[X(T)]

lδ~(1) _{l\widetilde{\delta}} \tag{1}
R(gC)⟶chZ[P] \mathscr{R}(\mathfrak{g}_{\mathbf{C}})\longrightarrow^{ch}\mathbf{Z}[P]

where P denotes the group of weights of R(gC,tC)R(\mathfrak{g}_{\mathbf{C}},\mathfrak{t}_{\mathbf{C}}) and δ~\widetilde{\delta} the homomorphism induced by δ\delta.

The Weyl group W operates by automorphisms on the group X(T), and hence on the ring Z[X(T)]\mathbf{Z}[X(T)]. By Prop. 5 of §4, no. 3, the image of Ch is contained in the subring Z[X(T)]W\mathbf{Z}[X(T)]^W consisting of the elements invariant under W.

Proposition 2 01G8

The homomorphism Ch induces an isomorphism from R(G) to Z[X(T)]WZ[X(T)]^W.

For λ∈X++\lambda \in X_{++}, denote by [λ][\lambda ] the class in R(G) of the irreducible representation of highest weight λ\lambda. Since the family ([λ])λ∈X++([\lambda ])_{\lambda\in X_{++}} is a basis of the Z\mathbf{Z}-module R(G), it suffices to prove the following assertion:

The family (Ch[λ]\lambda ])λ∈X++_{\lambda\in X_{++}} is a basis of the Z\mathbf{Z}-module Z[X(T)]W\mathbf{Z}[X(T)]^W.

For every element u=∑λaλeλu=\sum_{\lambda}a_{\lambda}e^{\lambda} of Z[X(T)]\mathbf{Z}[X(T)], a term aλeλa_{\lambda}e^{\lambda} in uu is called maximal if λ\lambda is a maximal element of the set of μ∈X(T)\mu\in X(T) such that aμ≠0a_\mu\not= 0. Th. 1 implies that Ch[λ]\lambda ] has a unique maximal term, namely eλe^{\lambda}. Thus, the proposition follows from the following lemma.

Lemma 3 01G9

For each λ∈X++\lambda \in X_{++}, let CλC_{\lambda} be an element of Z[X(T)]W\mathbf{Z}[X(T)]^W having unique maximal term eλe^{\lambda}. Then the family (Cλ)λ∈X++(C_{\lambda})_{\lambda\in X_{++}} is a basis of Z[X(T)]W\mathbf{Z}[X(T)]^W.

The proof is identical to that of Prop. 3 of Chap. VI, §3, no. 4, replacing A by Z,P\mathbf{Z}, P by X(T) and P∩C‾P\cap \overline{C} by X++X_{++}.

Let Θ(G)\Theta (G) (resp. Θ(T)\Theta (T)) be the C\mathbf{C}-algebra of continuous representative functions on G (resp. T), and let ZΘ(G)Z\Theta (G) (resp. Θ(T)W\Theta (T)^W) be the subalgebra consisting of the central (resp. W-invariant) functions. The restriction map Θ(G)→Θ(T)\Theta (G)\rightarrow \Theta (T) induces a homomorphism of rings r:ZΘ(G)→Θ(T)Wr: Z\Theta (G)\rightarrow \Theta (T)^W. On the other hand, the map that associates to a representation τ\tau its character (that is, the function g→g \rightarrow Tr τ(g)\tau (g)) extends to a homomorphism of C\mathbf{C}-algebras Tr:C⊗ZR(G)→ZΘ(G):\mathbf{C}\otimes_{\mathbf{Z}}R(G)\rightarrow Z\Theta (G) which, by Spectral Theories, is an isomorphism. Similarly, the canonical injection X(T)→Θ(T)X(T)\rightarrow \Theta (T) induces an isomorphism of C\mathbf{C}-algebras ι:C[X(T)]→Θ\iota :\mathbf{C}[X(T)]\rightarrow \Theta(T), which induces an isomorphism ι:C[X(T)]W→Θ(T)W\iota :\mathbf{C}[X(T)]^W\rightarrow \Theta (T)^W. The diagram

C⊗ZR(G)⟶1⊗ChC[X(T)]W \mathbf{C}\otimes_{\mathbf{Z}}R(G)\overset{1\otimes Ch}{\longrightarrow}\mathbf{C}[X(T)]^W
Trι(2) _{Tr}^{\iota} \tag{2}
ZΘ(G)⟶rΘ(T)W Z\Theta (G)\longrightarrow^r\Theta (T)^W

is commutative: indeed, for every representation τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) and all t∈Tt\in T,

Tr τ(t)=∑λ∈X(T)\tau (t) =\sum_{\lambda\in X(T)}(dim Vλ(T)V_{\lambda}(T))λ(t)=ι\lambda (t) =\iota(Chτ\tau )(t)(t),

that is, (r∘(r\circ Tr)[τ]=(ι∘\tau ] = (\iota \circ Ch)[τ]\tau ].

We can now deduce from the proposition the following result.

Corollary 01GA

The restriction map r:ZΘ(G)→Θ(T)Wr: Z\Theta (G)\rightarrow \Theta (T)^W is bijective.

4. Character formula

In this number, we write the group X(T) multiplicatively, and regard its elements as complex-valued functions on T. We assume that the element ρ\rho of X(T)⊗QX(T)\otimes \mathbf{Q} belongs to X(T).

Denote by L2(T)L^2(T) the Hilbert space of classes of square-integrable complex functions on T, and by Θ(T)\Theta (T) the subspace consisting of the continuous representative functions. By Spectral Theories, X(T) is an orthonormal basis of L2(T)L^2(T) and an algebraic basis of Θ(T)\Theta (T).

For f∈L2(T)f\in L^2(T) and w∈Ww\in W, denote by wf^wf the element of L2(T)L^2(T) defined by wf(t)=f(w−1(t))^wf(t) =f(w^{-1}(t)); thus, for λ∈X(T)\lambda \in X(T) we have wλ=w(λ)^w\lambda =w(\lambda ). Denote by ε:W→{1,−1}\varepsilon : W\rightarrow \{1,-1\} the signature (the unique homomorphism such that ε(s)=\varepsilon (s) = −1-1 for every reflection ss); for f∈L2f\in L^2(T), put

J(f)=∑w∈Wε(w)wf J(f) =\sum_{w\in W}\varepsilon (w)^wf

If λ∈X++\lambda \in X_{++}, the characters w(λρ)^w(\lambda \rho ) are distinct; indeed, it suffices to prove that w(λρ)≠λρ^w(\lambda \rho )\not=\lambda \rho for all w≠1w\not= 1; but this follows from Lemma 1 (no. 1) and the fact that ⟨λρ,Kα⟩=⟨λ,Kα⟩+1>0\langle \lambda \rho , K_{\alpha}\rangle =\langle \lambda , K_{\alpha}\rangle + 1>0 for every positive root α\alpha. Consequently,

∥J(λρ)∥2=\|J(\lambda \rho )\|^2= Card(W) =w(G)=w(G).

An element f∈L2(T)f\in L^2(T) is said to be anti-invariant if wf=ε(w)f^wf=\varepsilon (w)f for all w∈Ww\in W (that is, if sf=−f^sf=-f for every reflection ss). We shall show that 1w(G)J\frac{1}{w(G)}J is the orthogonal projection of L2(T)L^2(T) onto the subspace of anti-invariant elements. Indeed, let f,f′f, f' be in L2L^2(T), with f′f' anti-invariant; then J(f)J(f) is anti-invariant and

⟨f′,J(f)⟩=∑w∈Wε(w)⟨f′,wf⟩=∑w∈W⟨wf′,wf⟩ \langle f',J(f)\rangle =\sum_{w\in W}\varepsilon (w)\langle f',^wf\rangle =\sum_{w\in W}\langle^wf',^wf\rangle
=∑w∈W⟨f′,f⟩=w(G)⟨f′,f⟩ =\sum_{w\in W}\langle f', f\rangle =w(G)\langle f', f\rangle

Proposition 3 01GB

The elements J(λρ)/√w(G)‾J(\lambda \rho )/\surd\overline{w(G)}, for λ∈X++\lambda \in X_{++}, form an orthonormal basis of the subspace of anti-invariant elements of L2(T)L^2(T), and an algebraic basis of the subspace of anti-invariant elements of Θ(T)\Theta (T).

The proof is identical to that of Chap. VI, §3, no. 3, Prop. 1.

By Chap. VI, loc. cit., Prop. 2,

J(ρ)=ρ∏α>0(1−α−1)=ρ−1∏α>0(α−1)(3) J(\rho ) =\rho \prod_{\alpha >0}(1-\alpha^{-1}) =\rho^{-1}\prod_{\alpha >0}(\alpha -1) \tag{3}

so

J(ρ)J(ρ)=∏α(α−1)(4) J(\rho )J(\rho ) =\prod_{\alpha}(\alpha -1) \tag{4}

By Cor. 2 of Th. 1 (§6, no. 2), we deduce:

Lemma 4 01GC

If φ\varphi and ψ\psi are two continuous central functions on G,

∫Gφ(g)‾ψ(g)dg=1w(G)∫T(φ(t)J(ρ)(t))‾.(ψ(t)J(ρ)(t))dt \int_G\overline{\varphi(g)}\psi (g)dg=\frac{1}{w(G)}\int_T\overline{(\varphi(t)J(\rho)(t))}.(\psi (t)J(\rho )(t))dt

For all λ∈X++\lambda \in X_{++}, denote by χλ\chi_{\lambda} the character of an irreducible representation of G of highest weight λ\lambda.

Theorem 2 (H. Weyl) 01GD

For all λ∈X++\lambda \in X_{++}, we have J(ρ).χλ∣T=J(λρ)J(\rho ).\chi_{\lambda}|T = J(\lambda \rho ).

The function J(ρ).χλ∣TJ(\rho ).\chi_{\lambda}|T is anti-invariant under W, and is a linear combination with integer coefficients of elements of X(T). Thus, by Chap. VI, §3, no. 3, Prop. 1, it can be written as ∑μaμJ(μρ)\sum_\mu a_\mu J(\mu\rho ), where μ\mu belongs to X++X_{++}, and the aμa_\mu are integers all but finitely-many of which are zero; since ∫G∣χλ(g)∣2dg=1\int_G|\chi_{\lambda}(g)|^2dg= 1

(Spectral Theories), it follows from Prop. 3 and Lemma 4 that ∑μ(aμ)2=1\sum_\mu(a_\mu)^2= 1; thus, the aμa_\mu are all zero, except one which must be equal to 1 or −1-1. But the coefficient of λ\lambda in χα∣T\chi_{\alpha}|T is equal to 1 (Th. 1), hence the coefficient of λρ\lambda \rho in J(ρ).χλ∣TJ(\rho ).\chi_{\lambda}|T is equal to 1 (Chap. VI, §3, no. 3, Remark 2), which implies that aλρ=1a_{\lambda \rho}= 1, hence the theorem.

Corollary 1 01GE

With the notations of no. 3, we have in Z[X(T)]\mathbf{Z}[X(T)],

(∑w∈Wε(w)ewρ)(\sum_{w\in W}\varepsilon (w)e^{w\rho}) Ch[λ]=∑w∈Wε(w)ewλewρ\lambda ] =\sum_{w\in W}\varepsilon (w)e^{w\lambda}e^{w\rho} for all λ∈X++\lambda \in X_{++}.

This follows from the theorem and commutative diagram (2) (no. 3).

Corollary 2 01GF

For all λ∈X++\lambda \in X_{++} and every regular element tt of T,

χλ(t)=∑∑wεw(wε)(λw()wtρ()wtρ()wt)(5) \chi_{\lambda}(t) =\sum\sum^w\varepsilon_w(w\varepsilon )(\lambda w()wt\rho ()wt\rho ()wt) \tag{5}

where the two sums are over the elements ww of W.

Indeed, J(ρ)(t)J(\rho )(t) is non-zero, since tt is regular (formula (4)).

If φ\varphi is a central function on G, the restriction of φ\varphi to T is invariant under W, so J(ρ).φ∣TJ(\rho ).\varphi |T is anti-invariant under W. Further, by Spectral Theories and Th. 1, the family (χλ)λ∈X++(\chi_{\lambda})_{\lambda\in X_{++}} is an algebraic basis of the space of central representative functions on G and an orthonormal basis of the space ZL2(G)^2(G) of classes of square-integrable central functions on G.

Thus, from Prop. 3 and Th. 2 we deduce:

Corollary 3 01GG

The map which associates to any continuous central function φ\varphi on G the function w(G)−1/2J(ρ)(φ∣T)w(G)^{-1/2}J(\rho )(\varphi |T) induces an isomorphism from the space of central representative functions on G to the space of anti-invariant elements of Θ(T)\Theta (T); it extends by continuity to an isomorphism of Hilbert spaces from ZL2(G)^2(G) to the subspace of anti-invariant elements of L2(T)L^2(T).

Corollary 4 01GH

Let φ\varphi be a continuous central function on G. Then,

∫Gχλ(g)‾φ(g)dg=∫Tλ(t)‾∏α>0(1−α(t)−1)φ(t)dt=∫Tλρ(t)‾.φ(t)J(ρ)(t)dt \int_G\overline{\chi_{\lambda}(g)}\varphi (g)dg=\int_T\overline{\lambda(t)}\prod_{\alpha >0}(1-\alpha (t)^{-1})\varphi (t)dt=\int_T\overline{\lambda \rho(t)}.\varphi (t)J(\rho )(t)dt

Indeed, by Lemma 4 and Th. 2,

∫Gχλ(g)‾φ(g)dg=1w(G)∫Tχλ(t)J(ρ)(t)(φ(t)J(ρ)(t))dt \int_G\overline{\chi_{\lambda}(g)}\varphi (g)dg=\frac{1}{w(G)}\int_T\chi_{\lambda}(t)J(\rho )(t)(\varphi (t)J(\rho )(t))dt
=1w(G)∫TJ(λρ)(t)‾φ(t)J(ρ)(t)dt =\frac{1}{w(G)}\int_T\overline{J(\lambda \rho)(t)}\varphi (t)J(\rho )(t)dt

But the function t→φ(t)J(ρ)(t)t \rightarrow \varphi (t)J(\rho )(t) is anti-invariant and 1w(G)J(λρ)\frac{1}{w(G)}J(\lambda \rho ) is the orthogonal projection of λρ\lambda \rho onto the subspace of anti-invariant elements of L2L^2(T), so

1w(G)∫TJ(λρ)(t)‾φ(t)J(ρ)(t)dt=∫Tλρ(t)‾φ(t)J(ρ)(t)dt \frac{1}{w(G)}\int_T\overline{J(\lambda \rho)(t)}\varphi (t)J(\rho )(t)dt=\int_T\overline{\lambda \rho(t)}\varphi (t)J(\rho )(t)dt

finally, by formula (3), we have ρ(t)J(ρ)(t)=∏α>0(1−α(t)−1)\rho (t)J(\rho )(t) =\prod_{\alpha >0}(1-\alpha (t)^{-1}), hence the corollary.

Remark 1 01GI

For all w∈Ww\in W, put ρw=wρ/ρ\rho_w=^w\rho /\rho; then

∑wε(w)ρw=∏α>0(1−α−1)=ρ−2∏α>0(α−1)(6) \sum_w\varepsilon (w)\rho_w=\prod_{\alpha >0}(1-\alpha^{-1}) =\rho^{-2}\prod_{\alpha >0}(\alpha -1) \tag{6}

If tt is a regular element of T, we deduce from (5) that

χλ(t)=∑∑wεw(wε)(wwλ)ρ(tw)(ρtw)(t)=∑∏α>wε(0w(1)−wλα(t()tρ)w−(1t))(7) \chi_{\lambda}(t) =\sum\sum^w\varepsilon_w(w\varepsilon )(\overset{w}{w}\lambda )\rho (t_w)(\rho t^w)(t)=\sum\prod^w_{\alpha >}\varepsilon (_0w(1)\overset{w}{-}\lambda \alpha (t()t\rho )^{w-}(_1t)) \tag{7}

Note that ρw\rho_w is a linear combination of roots with integer coefficients, and hence belongs to X(T) even if we do not assume that ρ∈X(T)\rho \in X(T). It follows that formula (7) is valid without the assumption that ρ∈X(T):\rho \in X(T): indeed, to prove this we replace G by a suitable connected covering, and are then reduced to Cor. 2.

Remark 2 01GJ

Similarly, the first equality of Cor. 4 remains valid without the assumption that ρ∈X(T)\rho \in X(T).

Remark 3 01GK

We can deduce Th. 2 from the analogous infinitesimal statement (Chap. VIII, §9, no. 1, Th. 1); the same is true for Th. 3 of the next number (which is the analogue of Th. 2 of loc. cit., no. 2).

5. Degree of irreducible representations

We now return to the additive notation for the group X(T) and we no longer assume that ρ\rho belongs to X(T).

Theorem 3 01GL

The dimension of the space of an irreducible representation of G of highest weight λ\lambda is given by

χλ(e)=∏α∈R+⟨λ+ρ,Kα⟩⟨ρ,Kα⟩ \chi_{\lambda}(e) =\prod_{\alpha\in R_+}\frac{\langle\lambda + \rho , K_{\alpha}\rangle}{\langle\rho , K_{\alpha}\rangle}

Put γ=12∑α>0Kα\gamma =\frac{1}{2}\sum_{\alpha >0}K_{\alpha}, so δ(α)(γ)=2πi\delta (\alpha )(\gamma ) = 2\pi i for every simple root α\alpha (Chap. VI, §1, no. 10, Prop. 29). The line Rγ\mathbf{R}\gamma is not contained in any of the hyperplanes Ker δ(α)\delta (\alpha ), so exp(zγz\gamma ) is a regular element of G for all sufficiently small z∈R∗z\in \mathbf{R}^*; for all μ∈X(T)\mu\in X(T) and all z∈Rz\in \mathbf{R}, we have

J(μJ(\mu)(exp(zγz\gamma )) =∑w∈Wε(w)ezδ(μ)(w−1γ)=\sum_{w\in W}\varepsilon (w)e^{z\delta(\mu)(w^{-1}\gamma)}.

Let us accept provisionally the following lemma:

Lemma 5 01GM

We have

J(μJ(\mu)(exp(zγz\gamma )) =ezδ(μ)(γ)∏α>0(1−e−zδ(μ)(Kα))=e^{z\delta(\mu)(\gamma)}\prod_{\alpha >0}(1-e^{-z\delta(\mu)(K_{\alpha})}).

Thus, the function J(μJ(\mu)(exp(zγz\gamma )) is the product of a function that tends to 1 when zz tends to 0 and of

zN∏α>0δ(μ)(Kα)=(2πiz)N∏α>0⟨μ,Kα⟩ z^N\prod_{\alpha >0}\delta (\mu)(K_{\alpha}) = (2\pi iz)^N\prod_{\alpha >0}\langle \mu, K_{\alpha}\rangle

where N = Card R+R_+.

Assume first of all that ρ∈X(T)\rho \in X(T); applying Cor. 2 of Th. 2 we see that, as zz tends to 0,χλ(zγ)0,\chi_{\lambda}(z\gamma ) tends to

∏α>0⟨λ+ρ,Kα⟩/∏α>0⟨ρ,Kα⟩ \prod_{\alpha >0}\langle \lambda +\rho , K_{\alpha}\rangle /\prod_{\alpha >0}\langle \rho , K_{\alpha}\rangle

hence the theorem in this case.

In the general case, it suffices to remark that, in proving Th. 3, we can always replace G by a suitable connected covering and thus reduce to the preceding case.

We now prove Lemma 5. Let z∈Cz\in \mathbf{C}; denote by φz\varphi_z the map from t\mathfrak{t} to the C\mathbf{C}-algebra Map(X(T),C,\mathbf{C}) of maps from X(T) to C\mathbf{C} that associates to H∈tH\in \mathfrak{t} the map

φz(H):μ→μ\varphi_z(H) :\mu \rightarrow \mu(exp zHzH) =ezδ(μ)(H)=e^{z\delta(\mu)(H)}.

We have φz(H+H′)=φz(H)φz(H′)\varphi_z(H+H') =\varphi_z(H)\varphi_z(H'), so there exists a homomorphism of rings

ψz:Z[t]→\psi_z:\mathbf{Z}[\mathfrak{t}]\rightarrow Map(X(T),C,\mathbf{C})

such that ψz(eH)(μ)=ezδ(μ)(H)\psi_z(e^H)(\mu) =e^{z\delta(\mu)(H)}. On the other hand, by Chap. VI, §3, no. 3, Prop. 2, we have the following relation in Z[t]:\mathbf{Z}[\mathfrak{t}]:

∑w∈Wε(w)ewγ=eγ∏α>0(1−e−Kα) \sum_{w\in W}\varepsilon (w)e^{w\gamma}=e^{\gamma}\prod_{\alpha >0}(1-e^{-K_{\alpha}})

Applying the homomorphism ψz\psi_z, and using the equality

ψz(ewγ)(μ)=ezδ(μ)(wγ)=ezδ(w−1μ)(γ) \psi_z(e^{w\gamma})(\mu) =e^{z\delta(\mu)(w\gamma)}=e^{z\delta(w^{-1}\mu)(\gamma)}

we deduce the stated formula.

Corollary 1 01GN

Let ∥∥\| \| be a norm on X(T)⊗RX(T)\otimes \mathbf{R}. For all λ∈X++\lambda \in X_{++}, let d(λ)d(\lambda ) be the dimension of the space of an irreducible representation of G of highest weight λ\lambda.

a) supλ∈X++d(λ)/∥λ+ρ∥N<∞_{\lambda\in X_{++}}d(\lambda )/\|\lambda +\rho \|^N<\infty, where N=1/N = 1/2(dim G−G- dim T).

b) If G is semi-simple, infλ∈X++d(λ)/∥λ+ρ∥>0_{\lambda\in X_{++}}d(\lambda )/\|\lambda +\rho \|>0.

a) For all α∈R+\alpha \in R_+, there exists Aα>0A_{\alpha}>0 with ∣⟨λ+ρ,Kα⟩∣≤Aα∥λ+ρ∥|\langle \lambda +\rho , K_{\alpha}\rangle | \leq A_{\alpha}\|\lambda +\rho \|, hence d(λ)/∥λ+ρ∥N≤∏α>0Aα/⟨ρ,Kα⟩d(\lambda )/\|\lambda +\rho \|^N\leq \prod_{\alpha >0}A_{\alpha}/\langle \rho , K_{\alpha}\rangle.

b) Assume that G is semi-simple, denote by β1,...,βr\beta_1, . . . , \beta_r the simple roots and put Ni=KβiN_i=K_{\beta_i}. Then

d(λ)≥∏i=1r⟨λ+ρ,Ni⟩⟨ρ,Ni⟩=∏i=1r⟨λ+ρ,Ni⟩ d(\lambda )\geq \prod_{i=1}^r\frac{\langle\lambda + \rho , N_i\rangle}{\langle\rho , N_i\rangle}=\prod_{i=1}^r\langle \lambda +\rho , N_i\rangle

since ⟨λ+ρ,Ni⟩≥⟨ρ,Ni⟩=1\langle \lambda +\rho , N_i\rangle \geq \langle \rho , N_i\rangle = 1, this implies that

d(λ)≥d(\lambda )\geq supi∣⟨λ+ρ,Ni⟩∣_i|\langle \lambda +\rho , N_i\rangle |.

If G is semi-simple, x→x \rightarrow sup∣⟨x,Ni⟩∣|\langle x, N_i\rangle | is a norm on X(T)⊗RX(T)\otimes \mathbf{R}, necessarily equivalent to the given norm, hence b).

Corollary 2 01GO

Assume that G is semi-simple; let dd be an integer. The set of classes of representations of G of dimension ≤d\leq d is finite.

Cor. 1b)1b) implies that the set XdX_d of elements λ\lambda of X++X_{++} such that d(λ)≤dd(\lambda )\leq d is finite. For all λ\lambda in XdX_d, let VλV_{\lambda} be an irreducible representation of highest weight λ\lambda; every representation of dimension ≤d\leq d is isomorphic to a direct sum ⨁λ∈XdVλnλ\bigoplus_{\lambda\in X_d}V^{n_{\lambda}}_{\lambda}, with nλ≤dn_{\lambda}\leq d, hence the corollary.

6. Casimir elements

By Prop. 3 of §1, no. 3, there exist negative symmetric bilinear forms on g\mathfrak{g}, separating and invariant under Ad(G) (if G is semi-simple, we can take the Killing form of g\mathfrak{g}, for example). Let F be such a form. Recall (Chap. I, §3, no. 7) that the Casimir element associated to F is the element Γ\Gamma of the centre of the enveloping algebra U(g)U(\mathfrak{g}) such that, for any basis (ei)(e_i) of g\mathfrak{g} satisfying F(ei,ej)=−δijF(e_i, e_j) =-\delta_{ij}, we have Γ=−∑ei2\Gamma =-\sum e^2_i.

In the remainder of this chapter we shall call the Casimir elements of G the elements of U(g)U(\mathfrak{g}) obtained in this way from negative separating invariant symmetric bilinear forms on g\mathfrak{g}. If Γ\Gamma is a Casimir element of G and if τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) is an irreducible representation of G, the endomorphism ΓV\Gamma_V of V is a homothety (Algebra, Chap. VIII, §3, no. 2, Th. 1), whose ratio we shall denote by Γ~(τ)\widetilde{\Gamma}(\tau ).

Proposition 4 01GP

Let Γ\Gamma be the Casimir element of G.

a) If τ\tau is an irreducible representation of G,Γ~(τ),\widetilde{\Gamma}(\tau ) is real and positive. If τ\tau is not the trivial representation, Γ~(τ)>0\widetilde{\Gamma}(\tau )>0.

b) There exists a unique quadratic form QΓQ_{\Gamma} on X(T)⊗RX(T)\otimes \mathbf{R} such that, for every irreducible representation τ\tau of G,

Γ~(τ)=QΓ(λ+ρ)−QΓ(ρ) \widetilde{\Gamma}(\tau ) = Q_{\Gamma}(\lambda +\rho )-Q_{\Gamma}(\rho )

where λ\lambda is the highest weight of τ\tau. The form QΓQ_{\Gamma} is positive, separating and invariant under W.

Let F be a separating negative symmetric bilinear form on g\mathfrak{g} defining Γ\Gamma. Let τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) be an irreducible representation of G; let ⟨,⟩\langle ,\rangle be a Hilbert scalar product on V invariant under G (§1, no. 1), and (ei)(e_i) a basis of g\mathfrak{g} such that F(ei,ej)=−δijF(e_i, e_j) =-\delta_{ij}. Then, for every element vv of V not invariant under G we have

Γ~(τ)⟨v,v⟩=⟨v,ΓV(v)⟩=−∑i⟨v,(ei)V2v⟩=∑i⟨v,(ei)V∗(ei)Vv⟩ \widetilde{\Gamma}(\tau )\langle v, v\rangle =\langle v, \Gamma_V(v)\rangle =-\sum_i\langle v,(e_i)^2_Vv\rangle =\sum_i\langle v,(e_i)^*_V(e_i)_Vv\rangle
=∑i⟨(ei)Vv,(ei)Vv⟩>0 =\sum_i\langle (e_i)_Vv,(e_i)_Vv\rangle >0

hence a).

Let B be the inverse form on tC∗\mathfrak{t}^*_{\mathbf{C}} of the restriction to tC\mathfrak{t}_{\mathbf{C}} of the bilinear form on gC\mathfrak{g}_{\mathbf{C}} induced by F by extension of scalars. By the Cor. of Prop. 7 of Chap. VIII, §6, no. 4, we have5Γ~(τ)=B(δ(λ),δ(λ+2ρ))^5\widetilde{\Gamma}(\tau ) = B(\delta (\lambda ), \delta (\lambda +2\rho )). Extend δ:X(T)→\delta : X(T)\rightarrow tC∗\mathfrak{t}^*_{\mathbf{C}} to an R\mathbf{R}-linear map from X(T)⊗RX(T)\otimes \mathbf{R} to tC∗\mathfrak{t}^*_{\mathbf{C}} and let QΓQ_{\Gamma} be the quadratic form x→B(δ(x),δ(x))x \rightarrow B(\delta (x), \delta (x)) on X(T)⊗RX(T)\otimes \mathbf{R}; it is separating and invariant under W, and

Γ~(τ)=B(δ(λ+ρ),δ(λ+ρ))−B(δ(ρ),δ(ρ))=QΓ(λ+ρ)−QΓ(ρ) \widetilde{\Gamma}(\tau ) = B(\delta (\lambda +\rho ), \delta (\lambda +\rho ))-B(\delta (\rho ), \delta (\rho )) = Q_{\Gamma}(\lambda +\rho )-Q_{\Gamma}(\rho )

We show that the form QΓQ_{\Gamma} is positive. Indeed, if x∈X(T)⊗Qx\in X(T)\otimes \mathbf{Q}, the element δ(x)\delta (x) of tC∗\mathfrak{t}^*_{\mathbf{C}} takes purely imaginary values on t\mathfrak{t}, hence real values on iti\mathfrak{t}; we conclude by remarking that, for y∈ity\in i\mathfrak{t}, we have F(y,y)≥0F(y, y)\geq 0.

It remains to prove the uniqueness assertion in b). Let Q be a quadratic form on X(T)⊗RX(T)\otimes \mathbf{R} satisfying the required condition, and let Φ\Phi (resp. ΦΓ\Phi_{\Gamma}) be the bilinear form associated to Q (resp. QΓQ_{\Gamma}). For λ,μ∈X++\lambda , \mu\in X_{++}, we have

Φ(λ,μ)=(Q(λ+μ+ρ)−Q(ρ))−(Q(λ+ρ)−Q(ρ))−(Q(μ+ρ)−Q(ρ)) \Phi (\lambda , \mu) = (Q(\lambda +\mu+\rho )-Q(\rho ))-(Q(\lambda +\rho )-Q(\rho ))-(Q(\mu+\rho )-Q(\rho ))
=ΦΓ(λ,μ) =\Phi_{\Gamma}(\lambda , \mu)

Since X(T)++X(T)_{++} generates the R\mathbf{R}-vector space X(T)⊗RX(T)\otimes \mathbf{R}, we have Φ=ΦΓ\Phi =\Phi_{\Gamma}, so Q=QΓQ = Q_{\Gamma}.

Remark 01GQ

Let x∈gx\in \mathfrak{g}. There exists a strictly positive real number A such that, for every irreducible representation τ:G→GL(V)\tau : G\rightarrow \mathbf{G}\mathbf{L}(V) and every Hilbert structure on V invariant under G,

∥L(τ)(x)∥2≤A.Γ~(τ) \|L(\tau )(x)\|^2\leq A.\widetilde{\Gamma}(\tau )

Indeed, with the notations in the preceding proof, we can choose the basis (ei)(e_i) of g\mathfrak{g} so that x=ae1,a∈Rx=ae_1,a\in \mathbf{R}. Then, for v∈Vv\in V, we have

⟨xVv,xVv⟩=∣a∣2⟨e1v,e1v⟩≤∣a∣2Γ~(τ)⟨v,v⟩ \langle x_Vv, x_Vv\rangle =|a|^2\langle e_1v, e_1v\rangle \leq |a|^2\widetilde{\Gamma}(\tau )\langle v, v\rangle

Exercises

See the exercises for § 7.

Transcribed from the printed volume. Not translated.