§ 9. The formula of hermann Weyl
In this paragraph, we retain the general notations of §6 and §7.
1. Characters of finite dimensional g-modules
Let (eλ)λ∈h∗ be the canonical basis of the ring Z[h∗]. Give the space Zh∗ of all maps from h∗ to Z the product topology of the discrete topologies on the factors. If φ∈Zh∗, the family (φ(ν)eν)ν∈h∗ is summable, and
φ=ν∈h∗∑φ(ν)eν
Let Z⟨P⟩ be the set of φ∈Zh∗ whose support is contained in a finite union of sets of the form ν−P+, where ν∈h∗. Then Z[P]⊂Z⟨P⟩⊂Zh∗. Define on Z⟨P⟩ a ring structure extending that of Z[P] by putting, for φ,ψ∈Z⟨P⟩ and ν∈h∗,
(φψ)(ν)=μ∈h∗∑φ(μ)ψ(ν−μ)
(the family (φ(μ)ψ(ν−μ))μ∈h∗ has finite support, in view of the condition satisfied by the supports of φ and ψ ). If φ=∑νxνeν and ψ=∑νyνeν, then φψ=∑ν,μxνyμeν+μ.
Let ν∈h∗. A partition of ν into positive roots is a family (nα)α∈R+, where the nα are integers ≥0 such that ν=∑α∈R+nαα. We denote by P(ν) the number of partitions of ν into positive roots. We have
P(ν)>0⇐⇒ν∈Q+
In this paragraph, we denote by K the following element of Z⟨P⟩:
K=γ∈Q+∑P(γ)e−γ
Now recall (Chap. VI, §3, no. 3, Prop. 2) that
d=α∈R+∏(eα/2−e−α/2)=w∈W∑ε(w)ewρ
is an anti-invariant element of Z[P].
In the ring Z⟨P⟩, we have K.∏α∈R+(1−e−α)=Ke−ρd=1.
Indeed,
K=α∈R+∏(e0+e−α+e−2α+⋯)
so
Ke−ρd=α∈R+∏(1+e−α+e−2α+⋯)α∈R+∏(1−e−α)=1
Let λ∈h∗. The module Z(λ)(§6, no. 3) admits a character that is an element of Z⟨P⟩, and we have d. ch Z(λ)=eλ+ρ.
Let α1,...,αq be distinct elements of R+. The X−α1n1X−α2n2...X−αqnq⊗1 form a basis of Z(λ)(§6, Prop. 6 (iii)). For h∈h, we have
h.(X−α1n1X−α2n2...X−αqnq⊗1)
=[h,X−α1n1...X−αqnq]⊗1+(X−α1n1...X−αqnq)⊗h.1
=(λ−n1α1−⋯−nqαq)(h)(X−α1n1...X−αqnq⊗1)
Thus, the dimension of Z(λ)λ−μ is P(μ). This proves that ch Z(λ) is defined, is an element of Z⟨P⟩, and that
ch Z(λ)=∑μP(μ)eλ−μ=Keλ.
It now suffices to apply Lemma 1.
Let M be a g-module which admits a character ch(M) whose support is contained in a finite union of the sets μ−P+. Let U be the enveloping algebra of g, Z the centre of U,λ0∈h∗, and χλ0 the corresponding homomorphism from Z to k(§8, Cor. 1 of Th. 2). Assume that, for all z∈Z,zM is the homothety with ratio χλ0(z). Let DM be the set of λ∈W(λ0+ρ)−ρ such that λ+Q+ meets Supp(ch M). Then ch(M) is a Z-linear combination of the ch Z(λ) for λ∈DM.
If Supp(ch M) is empty, the lemma is clear. Assume that Supp(ch M)=∅. Let λ be a maximal element of this support, and put dim Mλ=m. There exists a g-homomorphism φ from (Z(λ))m to M which maps (Z(λ)λ)m bijectively onto Mλ(§6, no. 3, Prop. 6 (i)). Thus, the central character of Z(λ) is χλ0, so λ∈W(λ0+ρ)−ρ(§8, no. 5, Cor. 1 of Th. 2). This proves that DM=∅, and allows us to argue by induction on Card DM. Let L and N be the kernel and cokernel of φ. Then we have an exact sequence of g-homomorphisms:
0→L→(Z(λ))m→M→N→0
so
ch(M) =−ch(L) +m ch Z(λ)+ ch(N)
(§7, no. 7, formula (6)). The sets Supp(ch L) and Supp(ch N) are contained in a finite union of sets μ−P+. For z∈Z,zL and zN are homotheties with ratio χλ0(z). Clearly, DN⊂DM. On the other hand, (λ+Q+)∩Supp(ch M) ={λ}, and λ∈/ Supp(ch N), so λ∈/DN and
Card DN< Card DM.
On the other hand, L is a submodule of (Z(λ))m; if λ′∈DL, then λ′+Q+ meets Supp(ch L)⊂ Supp ch Z(λ), so λ∈λ′+Q+(§6, no. 1, Prop. 1 (ii)); it follows that DL⊂DM. Since L∩(Z(λ)λ)m=0, we have λ∈/DL, so
Card DL< Card DM.
It now suffices to apply the induction hypothesis.
Theorem 1 (Character Formula of H. Weyl) 015W
Let M be a finite dimensional simple g-module, and λ its highest weight. Then
(∑w∈Wε(w)ewρ).ch M=∑w∈Wε(w)ew(λ+ρ).
With the notations of Lemma 3, the central character of M is χλ(§6, no. 4, Prop. 7). Hence, by Lemmas 2 and 3,d.ch M is a Z-linear combination of the eμ+ρ such that
μ+ρ∈W(λ+ρ)
On the other hand, by §7, no. 7, Lemma 7,d.ch M is anti-invariant, and its unique maximal term is eλ+ρ, hence the theorem.
Take g=sl(2,k),h=kH. Let α be the root of (g,h) such that α(H)=2. The g-module V(m) has highest weight (m/2)α. Hence
ch(V(m)) =(e(m/2)α+21α−e−(m/2)α−21α)/(e21α−e−21α)
=e−(m/2)α.(e(m+1)α−1)/(eα−1)
=e−(m/2)α(emα+e(m−1)α+⋯+1)
=e(m/2)α+e(m−2)α/2+⋯+e−(m/2)α
which also follows easily from §1, no. 2, Prop. 2.
2. Dimensions of simple g-modules
If μ∈h∗, put J(eμ)=∑w∈Wε(w)ewμ, cf. Chap. VI, §3, no. 3.
Theorem 2 015Y
Let E be a finite dimensional simple g-module, λ its highest weight and (⋅∣⋅) a W-invariant non-degenerate positive symmetric bilinear form on h∗. Then:
∏⟨λ+ρ,Hα⟩∏((λ∣α))
dim E = = 1 +.
α∈R+⟨ρ,Hα⟩α∈R+(ρ∣α)
Let T be an indeterminate. For all ν∈P, denote by fν the homomorphism from Z[P] to R[[T]] that takes eμ to e(ν∣μ)T for all μ∈P. Then dim E is the constant term of the series fν(ch E).
For all μ,ν∈P, we have
fν(J(eμ))=w∈W∑ε(w)e(ν∣wμ)T
=w∈W∑ε(w)e(w−1ν∣μ)T=fμ(J(eν))
In particular, in view of Chap. VI, §3, no. 3, formula (3),
fρ(J(eμ))=fμ(J(eρ))=e(μ∣ρ)Tα∈R+∏(1−e−(μ∣α)T)
Hence, setting Card(R+) =N,
fρ(J(eμ))≡TN∏α∈R(μ∣α) (mod TN+1R[[T]]).
The equality J(eλ+ρ)= ch(E).J(eρ) (Th. 1) thus implies that
TN∏α∈R+(λ+ρ∣α)≡fρ(ch E).TN∏α∈R+(ρ∣α) (mod TN+1R[[T]])
so
dim E=((∏α∈R+(λ+ρ∣α))/((∏α∈R+(ρ∣α))=∏α∈R+(1+(ρ∣α)(λ∣α)).
Now, if α∈R+,α can be identified with an element of hR proportional to Hα, so
(λ+ρ∣α)/(ρ∣α)=⟨λ+ρ,Hα⟩/⟨ρ,Hα⟩
Example 1 015Z
In the Example of no. 1, we find that
dim V(m)=(2mα+2α)(Hα)/2α(Hα)=m+1,
which we knew in §1.
Example 2 0160
Take g to be the splittable simple Lie algebra of type G2 and adopt the notations of Chap. VI, Plate IX. Give hR∗ the W-invariant positive symmetric form (⋅∣⋅) such that (α1∣α1)=1. Then ρ=ϖ1+ϖ2 and
(ϖ1∣α1)=21,(ϖ1∣α2)=0,(ϖ1∣α2+α1)=21
(ϖ1∣α2+2α1)=1,(ϖ1∣α2+3α1)=23,(ϖ1∣2α2+3α1)=23
(ϖ2∣α1)=0,(ϖ2∣α2)=23,(ϖ2∣α2+α1)=23
(ϖ2∣α2+2α1)=23,(ϖ2∣α2+3α1)=23,(ϖ2∣2α2+3α1)=3
Thus, if n1,n2 are integers ≥0, the dimension of the simple representation of highest weight n1ϖ1+n2ϖ2 is
(1+12n1/2)((1+323n2/2)((1+12+23n1/2+3n2/2)((1+1+32n1+3n2/2)
×(1+32+233n1/2+3n2/2)((1+3n12/32+3+3n2)
=(1+n1)(1+n2)(1+4n1+3n2)((1+52n1+3n2)((1+2n1+n2)
×(1+3n1+2n2)
(1+n1)(1+n2)(2+n1+n2)(3+n1+2n2)(4+n1+3n2)(5+2n1+3n2)
=.
5!
In particular, the fundamental representation of highest weight ϖ1 (resp. ϖ2) is of dimension 7 (resp. 14).
3. Multiplicities of weights of simple g-modules
Proposition 1 0161
Let ω∈P++. For all λ∈P, the multiplicity of λ in E(ω) is
mλ=w∈W∑ε(w)P(w(ω+ρ)−(λ+ρ))
By Th. 1 and Lemma 1,
ch E(ω)=Ke−ρd ch E(ω)=Ke−ρ∑w∈Wε(w)ew(ω+ρ)
so
ch E(ω)=∑w∈W,γ∈Q+ε(w)P(γ)e−ρ+w(ω+ρ)−γ
and
mλ=∑ε(w)P(γ)
w∈W,γ∈Q+,γ=−λ−ρ+w(ω+ρ)
Corollary 0162
If λ is a weight of E(ω) distinct from ω,
mλ=−w∈W,w=1∑ε(w)mλ+ρ−wρ
Apply Prop. 1 with ω=0. If μ∈P-- {0}, we find that
0=w∈W∑ε(w)P(wρ+μ−ρ)
hence
P(μ)=−w∈W,w=1∑ε(w)P(μ+wρ−ρ)(1)
Prop. 1 also gives
mλ=−w∈W∑ε(w)w′∈W,w′=1∑ε(w′)P(w(ω+ρ)−(λ+ρ)+w′ρ−ρ)
since w(ω+ρ)=λ+ρ for all w∈W(§7, Prop. 5 (iii)). Hence,
mλ=−w′∈W,w′=1∑ε(w′)w∈W∑ε(w)P(w(ω+ρ)−(λ+ρ−w′ρ+ρ))
=−∑w′∈W,w′=1ε(w′)mλ+ρ−w′ρ (Prop.1).
4. Decomposition of tensor products of simple g-modules
Proposition 2 0163
Let λ,μ∈P++. In R(g), we have
[λ].[μ]=ν∈P++∑m(λ,μ,ν)[ν]
with
m(λ,μ,ν)=w,w′∈W∑ε(ww′)P(w(λ+ρ)+w′(μ+ρ)−(ν+2ρ))
Let E,F be finite dimensional simple g-modules of highest weights λ,μ. Let lν be the length of the isotypical component of E⊗F of highest weight ν. It suffices to show that
lν=w,w′∈W∑ε(ww′)P(w(λ+ρ)+w′(μ+ρ)−(ν+2ρ))(2)
Put c1= ch(E) =∑σ∈Pmσeσ,c2= ch(F), and d=J(eρ), where J is defined as in no. 2. We have ∑ξ∈P++lξch[ξ]= ch(E ⊗F) =c1c2
so, after multiplying by d and using Th. 1,
ξ∈P++∑lξJ(eξ+ρ)=c1J(eμ+ρ)=(σ∈P∑mσeσ)((w∈W∑ε(w)ew(μ+ρ))(3)
=τ∈P∑(w∈W∑ε(w)mτ+ρ−w(μ+ρ))eτ+ρ
Now, if ξ∈P++,ξ+ρ belongs to the chamber defined by B (Chap. VI, §1, no. 10); thus, for all w∈W distinct from 1, we have w(ξ+ρ)∈/P++. Consequently, the coefficient of eν+ρ in ∑ξ∈P++lξJ(eξ+ρ) is equal to lν. In view of (3), we obtain
lν=w∈W∑ε(w)mν+ρ−w(μ+ρ)
that is, by Prop. 1,
lν=w,w′∈W∑ε(w)ε(w′)P(w′(λ+ρ)−(ν+ρ−w(μ+ρ)+ρ))
which proves (2).
We return to the Example of no. 1. Let λ=(n/2)α,μ=(p/2)α, ν=(q/2)α with n≥p. We have
m(λ,μ,ν)=P(2nα+2α+2pα+2α−2qα−α)
−P(2nα+2α−2pα−2α−2qα−α)
−P(−2nα−2α+2pα+2α−2qα−α)
+P(−2nα−2α−2pα−2α−2qα−α)
=P(2n+p−qα)−P(2n−p−q−2α)
This is zero if n+p+q is not divisible by 2, or if q≥n+p. If
q=n+p−2r
with r an integer ≥0, we have
m(λ,μ,ν)=P(rα)−P((r−p−1)α)
hence m(λ,μ,ν)=1 if r≤p and m(λ,μ,ν)=0 if r>p. Finally, the g-module V(n)⊗V(p) is isomorphic to
V(n+p)⊕V(n+p−2)⊕V(n+p−4)⊕⋯⊕V(n−p)
(Clebsch-Gordan formula).
Exercises
All the g-modules considered are assumed to be finite dimensional.
See the exercises for § 9.