We retain the notations and conventions of the preceding paragraph.
5 The proof of loc. cit., which has been stated only for split semi-simple Lie algebras,
is valid without change in the case of split reductive Lie algebras.
1. Fourier transforms of integrable functions
In this number, we recall some definitions and results from Spectral Theories6.
Denote by G the set of classes of irreducible representations of G (on finite dimensional complex vector spaces). For all u∈G, denote by Eu the space of u and d(u) its dimension. There exist separating positive hermitian forms on Eu invariant under u, and any two such forms are proportional. Denote by A∗ (resp. ∥A∥∞) the adjoint (resp. the norm) of an element A of End(Eu) relative to one of these forms; for all g∈G, we have u(g)∗=u(g)−1=u(g−1) and ∥u(g)∥∞=1; for all x∈g, we have u(x)∗=−u(x)=u(−x).
Give End(Eu) the Hilbert space structure for which the scalar product is
⟨A∣B⟩=d(u)Tr(A∗B)=d(u)Tr(BA∗), (1)
and put
∥A∥2=⟨A∣A⟩1/2=(d(u)Tr(A∗A))1/2. (2)
We have
√d(u)∥A∥∞≤∥A∥2≤d(u)∥A∥∞(3)
so
∣⟨A∣B⟩∣≤d(u)2∥A∥∞∥B∥∞(4)
For all g∈G, we have ∥u(g)∥2=d(u).
Denote by F(G) the algebra ∏u∈G End(Eu). Denote by L2(G) the Hilbert sum of the Hilbert spaces End(Eu); this is the space of families A=(Au)∈F(G) such that ∑u∥Au∥22<∞, with the scalar product
⟨A∣B⟩=∑u∈G⟨Au∣Bu⟩=∑u∈Gd(u)Tr(Au∗Bu). (5)
Denote the Hilbert norm on L2(G) also by ∥∥2, so that ∥A∥22=∑u∈G∥Au∥22 for A∈L2(G).
If f is an integrable complex function on G, put
u(f)=∫Gf(g)u(g)dg∈ End(Eu) (6)
for all u∈G. We have ∥u(f)∥∞≤∫G∣f(g)∣dg=∥f∥1. The Fourier cotransform of f, denoted by F(f), is the family (u(f))u∈G∈F(G). If f∈L2(G),
6 See note 1, §7, p. 66.
∥f∥22=u∈G∑⟨u(f)∣u(f)⟩=∥F(f)∥22
so F induces an isometric linear map from the Hilbert space L2(G) to the Hilbert space L2(G): in other words, for f and f′ in L2(G), we have
For f and f′ in L1(G), the convolution product f∗f′ of f and f′ is defined by
(f∗f′)(h)=∫Gf(hg−1)f′(g)dg=∫Gf(g)f′(g−1h)dg
(the integral makes sense for almost all h∈G).
We have f∗f′∈L1(G) and, for all u∈G,u(f∗f′)=u(f)u(f′), so
F(f∗f′)=F(f).F(f′)(8)
Conversely, let A=(Au)u∈G be an element of F(G); for all u∈G, let FuA be the (analytic) function on G defined by
(FuA)(g)=⟨u(g)∣Au⟩=d(u)Tr(Auu(g)−1). (9)
If A∈L2(G), the family (FuA)u∈G is summable in L2(G); the Fourier transform of A, denoted by F(A), is the sum of this family. The maps F and F are inverse isomorphisms between the Hilbert spaces L2(G) and L2(G).
For all u∈G choose an orthonormal basis Bu of Eu, and denote by (uij(g)) the matrix of u(g) in this basis. Prop. 1 also means that the family of functions √d(u)uij, for u in G and i,j in Bu, is an orthonormal basis of the space L2(G).
If f is an integrable function on G such that the family (fu) is uniformly summable, then the sum of this family is a continuous function which coincides almost everywhere with f; in other words, if we assume in addition that f is continuous, then for all h∈G, f(h)=∑u∈Gd(u)∫Gf(gh)Tr(u(g))dg. (11)
Conversely, let A∈F(G); if the family (FuA)u∈G is uniformly summable, the function
g→∑u∈G(FuA)(g)=∑u∈Gd(u)Tr(Auu(g)−1)
is a continuous function on G whose Fourier cotransform is A.
Let f be an integrable function on G, and let s∈G. Denote by γ(s)f and δ(s)f the functions on G defined by γ(s)f=εs∗f,δ(s)f=f∗εs−1, that is,
(γ(s)f)(g)=f(s−1g),(δ(s)f)(g)=f(gs) for g∈G,
(Chap. III, §3, no. 4 and Integration, Chap. VII, §1, no. 1). We have
u(γ(s)f)=∫Gf(s−1g)u(g)dg=∫Gf(g)u(sg)dg
so
u(γ(s)f)=u(s)u(f)(12)
and similarly
u(δ(s−1)f)=u(f)u(s)(13)
When G is commutative, G is the underlying set of the dual group of G (Spectral Theories, Chap. II, §1, no. 1),d(u)=1 for all u∈G, and we recover the definitions of the Fourier transform given in Spectral Theories, Chap. II.
2. Fourier transforms of infinitely-differentiable functions
Recall (Chap. III, §3, no. 1, Def. 2) that U(G) denotes the algebra of distributions on G with support contained in {e}. The canonical injection of g into U(G) extends to an isomorphism from the enveloping algebra of the Lie algebra g to U(G) (loc. cit., no. 7, Prop. 25); from now on we identify these two algebras by this isomorphism. If f is an infinitely-differentiable complex function on G and if t∈U(G), we denote by Ltf and Rtf the functions on G defined by
Ltf(g)=⟨εg∗t,f⟩,Rtf(g)=⟨t∗εg,f⟩
(cf. loc. cit., no. 6). For all g∈G,
Lt∘γ(g)=γ(g)∘Lt,Rt∘δ(g)=δ(g)∘Rt
Let u∈G; denote by Eu the space of u. The morphism of Lie groups u:G→GL(Eu) gives by differentiation a homomorphism of (real) Lie algebras g→ End(Eu), hence a homomorphism of algebras, also denoted by u, from U(G) to End(Eu). If t∈U(G) and if f is an infinitely-differentiable function on G, then
u(Ltf)=u(f)u(t∨),u(Rtf)=u(t∨)u(f)(14)
where t∨ denotes the image of t under the principal anti-automorphism of U(G) (Chap. I, §2, no. 4); indeed, it suffices to verify this for t∈g, in which case it follows by differentiation from formulas (12) and (13) (cf. Chap. III, §3, no. 7, Prop. 27).
For all u∈G, denote by λ(u) the highest weight of u(§7, no. 2, Th. 1), so u→λ(u) is a bijective map from G to the set X++ of dominant elements of X(T).
Let Γ∈U(G) be a Casimir element of G (§7, no. 6); for all u∈G, the endomorphism u(Γ) of Eu is a homothety, whose ratio we denote by Γ(u), so we have a map u→Γ(u) from G to C.
If φ and ψ are two functions on G with positive real values, denote by “φ≼ψ” or “φ(u)≼ψ(u)” the relation “there exists M>0 such that φ(u)≤Mψ(u) for all u∈G”; this is a pre-order relation on the set of functions on G with positive real values.
Let m→∥m∥ be a norm on the R-vector space R⊗X(T) and Γ a Casimir element of G. Let φ be a function on G with positive real values.
a) The following conditions are equivalent:
(i) There exists an integer n>0 such that φ(u)≼(∥λ(u)∥+1)n (resp. for every integer n>0, we have φ(u)≼(∥λ(u)∥+1)−n).
(ii) There exists an integer n>0 such that φ(u)≼(Γ(u)+1)n (resp. for every integer n>0, we have φ(u)≼(Γ(u)+1)−n).
b) If G is semi-simple, conditions (i) and (ii) are also equivalent to:
(iii) There exists an integer n>0 such that φ(u)≼d(u)n (resp. for every integer n>0, we have φ(u)≼d(u)−n).
Note first of all that condition (i) is clearly independent of the choice of norm. Thus we can use the norm defined by the quadratic form QΓ associated to Γ(§7, no. 6, Prop. 4). Then
0≤Γ(u)=∥λ(u)+ρ∥2−∥ρ∥2
so Γ(u)+1≼(∥λ(u)∥+1)2≼Γ(u)+1, hence a).
Further, if G is semi-simple,
∥λ(u)+ρ∥≼d(u)≼∥λ(u)+ρ∥N, where N=1/2(dim G− dim T)
(§7, no. 5, Cor. 1 of Th. 3), so ∥λ(u)∥+1≼d(u)≼(∥λ(u)∥+1)N, hence b).
It follows from Prop. 2 that condition (i) is independent of the choice of maximal torus, chamber, and norm, and that condition (ii) is independent of the choice of Casimir element. A function φ satisfying conditions (i) and (ii) is said to be moderately increasing (resp. rapidly decreasing). The product of two moderately increasing functions is moderately increasing; the product of a moderately increasing function and a rapidly decreasing function is rapidly decreasing. If φ is rapidly decreasing, the family (φ(u))u∈G is summable.
The function u→d(u) is moderately increasing (§7, no. 5, Cor. 1 of Th. 3); for any norm ∥∥ on R⊗X(T), the function u→∥λ(u)∥ is moderately increasing. For any Casimir element Γ, the function u→Γ(u) is moderately increasing; more generally:
For all t∈ U(G), the functions u→∥u(t)∥∞ and u→∥u(t)∥2 on G are moderately increasing.
Since the product of two moderately increasing functions is moderately increasing, it suffices to prove this when t∈g: in that case the assertion follows from the Remark in §7, no. 6 and the inequality
a) Let f be an infinitely-differentiable complex function on G. Then the family (fu)u∈G, where fu(g)=⟨u(g)∣u(f)⟩, is uniformly summable on G and, for all h∈G,
b) Let f be an integrable function on G; then f is equal almost everywhere to an infinitely-differentiable function if and only if the function u→∥u(f)∥∞ is rapidly decreasing on G.
Let f be an infinitely-differentiable function on G, and let Γ be a Casimir element for G; by formula (14),
thus, the function u→∥u(f)∥∞ is indeed rapidly decreasing.
Conversely, let A=(Au)u∈G be an element of F(G) such that the function u→∥Au∥∞ is rapidly decreasing. Put fu(g)=⟨u(g)∣Au⟩; the function g→fu(g) is analytic, hence infinitely-differentiable. By Chap. III, §3, no. 7, Prop. 27,
(Lxfu)(g)=⟨u(g)u(x)∣Au⟩
for all x∈g. Let t∈U(G); by the preceding formula,
Since d(u) and ∥u(t)∥∞ are moderately increasing (Prop. 3) and ∥Au∥∞ is rapidly decreasing, the function u→ supg∣(Ltfu)(g)∣ is rapidly decreasing; thus, the family (Ltfu)u∈G is uniformly summable. It follows7 that the sum of the family (fu) is an infinitely-differentiable function on G, whose Fourier cotransform is (Au), hence the theorem.
Denote by S(G) the vector subspace of L2(G) consisting of the families A=(Au)u∈G such that the function u→∥Au∥∞ is rapidly decreasing on G. It follows from the theorem that the maps F:f→(u(f))u∈G and F:A→∑u∈G⟨u(g)∣Au⟩ induce inverse isomorphisms between the complex vector spaces C∞(G;C) and S(G). Give the space C∞(G;C) the topology of uniform C∞-convergence (§6, no. 4) which can be defined by the family of semi-norms f→ supg∈G∣Ltf(g)∣ for t∈U(G), and the space S(G) the topology defined by the sequence of semi-norms pn:A→ supu∈G(Γ(u)+1)n∥Au∥∞. Formula (15) of the preceding proof shows that F is continuous. Let t∈U(G), and let A=(Au)u∈G be an element of S(G); put fn(g)=⟨u(g)∣Au⟩. Let p be an integer such that ∑u∈GΓ(u)−p=M<∞. By the preceding proof, there exists a positive integer m such that, for all g∈G,
The maps F:f→(u(f))u∈G and F:A→∑u∈G⟨u(g)∣Au⟩ induce inverse isomorphisms between the topological vector spaces C∞(G;C) and S(G).
7 This follows from the fact that the space C∞(G;C), with the topology of uniform
C∞-convergence (§6, no. 4), is complete.
3. Fourier transforms of central functions
For all u∈G, denote by χu the character of u; thus,
χu(g)= Tr(u(g)),(g∈G). (16) Recall from Spectral Theory the formulas
χu∗χv=0(u,v∈G,u=v)(17)
χu∗χu=d(u)1χu(u∈G)(18)
For all u∈G, denote by εu the identity map of Eu. Recall (§7, no. 4) that ZL2(G) denotes the subspace of L2(G) consisting of the classes of the functions f that are central, that is, such that f∘ Int s=f for all s∈G, or equivalently that γ(s)f=δ(s−1)f for all s∈G.
Let f∈L2(G). Then f is central if and only if u(f) is a homothety for all u∈G. In that case
u(f)=d(u)εu∫Gf(g)χu(g)dg(19)
By Prop. 1 (no. 1), to say that f is central means that u(γ(s)f)=u(δ(s−1)f) for all s∈G and all u∈G; but this can also be written as u(s)u(f)=u(f)u(s) for all s∈G and all u∈G (formulas (12) and (13)), hence the first assertion of Prop. 4 (Schur’s lemma). If u(f) is a homothety, then u(f)=λuεu with
Conversely, if φ is a square-integrable complex function on G, the element (d(u)φ(u)εu)u∈G of F(G) belongs to L2(G), and we have (formula (9)) (Fu(d(u)φ(u)εu))(g)=d(u)Tr (d(u)φ(u)εuu(g)−1)=φ(u)χu(g),
so
F((d(u)φ(u)εu))=∑φ(u)χu(22)
u∈G
Note, in particular, that formulas (20) and (21) give, for u,v in G,8
Let f be a continuous central function on G. Then f is infinitely-differentiable if and only if the function u→∣⟨χu∣f⟩∣ is rapidly decreasing on G; in that case,
f(g)=u∈G∑⟨χu∣f⟩χu(g)
for all g∈G.
By Th. 1b), the function f is infinitely-differentiable if and only if the function u→∥u(f)∥∞ is rapidly decreasing; but, by (20),
∥u(f)∥∞=d(u)1∣⟨χu∣f⟩∣
hence the first assertion, since the functions d(u) and d(u)1 are moderately increasing.
Assume that f is infinitely-differentiable; by Th. 1a),f(g)=∑u∈Gfu(g) for all g∈G, so
Hence, f(g)=∑u∈G⟨χu∣f⟩χu(g); but, for all u∈G, the contragredient representation u′ of u satisfies χu=χu′ and the map u→u′ is a permutation of G; so we also have f(g)=∑u∈G⟨χu∣f⟩χu(g), hence the proposition.
8 We embed End(Eu) in the product F(G)=∏v∈G End(Ev) by associating to any
A∈ End(Eu) the family (Av)v∈G such that Au=A and Av=0 for v=u.
Let f be a continuous central function on G. Then f is infinitely-differentiable if and only if the restriction of f to T is infinitely-differentiable.
Indeed, by Cor. 4 of §7, no. 4,
⟨χu∣f⟩=∫Gλ(u)(t)φ(t)dt, where φ(t)=∏α>0(1−α(t)−1)f(t).
If f∣T is infinitely-differentiable, so is φ; by Prop. 5, applied to the group T, the function μ→∫Tμ(t)φ(t)dt on T=X(T) is then rapidly decreasing, and so is the function u→⟨χu∣f⟩; hence the function f is infinitely-differentiable (Prop. 5). The converse is clear.
4. Central functions on g and functions on t
Denote by C(G) the space of continuous complex-valued functions on G and by C∞(G) the subspace of infinitely-differentiable functions. Then we have a sequence of inclusions
Θ(G)⊂C∞(G)⊂C(G)⊂L2(G)
Denote by ZΘ(G),ZC∞(G),ZC(G), ZL2(G), respectively, the subspaces consisting of the central functions in these various spaces. Introduce similarly the spaces Θ(T),C∞(T),C(T),L2(T); for any space E in this list, denote by EW (resp. E−W) the subspace consisting of the invariant (resp. anti-invariant) elements for the operation of the Weyl group W. We have a commutative diagram
ZC(G)⟶acC(T)W
ZC∞(G)⟶a∞C∞(T)W
ZΘ(G)⟶aΘΘ(T)W
where the vertical arrows represent the canonical injections, and the maps ac,a∞,aΘ are induced by the restriction map from C(G) to C(T).
The maps ac,a∞,aΘ are bijective (§2, no. 5, Cor. 1 of Prop. 5, §8, no. 3, Cor. of Prop. 5, and §7, no. 3, Cor. of Prop. 2).
Assume now that the semi-sum ρ of the positive roots belongs to X(T) and consider the map b which to every continuous function φ on T associates φ.J(ρ). We have a commutative diagram
ZL2(G)−−−−−−−−−−−−−−−−−−−−⟶uL2(T)−W
ZC(G)⟶acC(T)W⟶bcC(T)−W
ZC∞(G)⟶a∞C∞(T)W⟶b∞C∞(T)−W
ZΘ(G)⟶aΘΘ(T)W⟶bΘΘ(T)−W
where the vertical arrows are the canonical inclusions, the maps bc,b∞,bΘ are induced by b, and u extends bc∘ac by continuity (§7, no. 4, Cor. 3 of Th. 2). The maps u and bΘ are bijective (loc. cit.); so is b∞ (Exerc. 5); on the other hand, bc is not surjective in general (Exerc. 6).