Bourbaki

§ 9. The formula of hermann Weyl

In this paragraph, we retain the general notations of §6 and §7.

1. Characters of finite dimensional g\mathfrak{g}-modules

Let (eλ)λ∈h∗(e^{\lambda})_{\lambda\in\mathfrak{h}^*} be the canonical basis of the ring Z[h∗]\mathbf{Z}[\mathfrak{h}^*]. Give the space Zh∗\mathbf{Z}^{\mathfrak{h}^*} of all maps from h∗\mathfrak{h}^* to Z\mathbf{Z} the product topology of the discrete topologies on the factors. If φ∈Zh∗\varphi \in \mathbf{Z}^{\mathfrak{h}^*}, the family (φ(ν)eν)ν∈h∗(\varphi (\nu )e^{\nu})_{\nu\in\mathfrak{h}^*} is summable, and

φ=∑ν∈h∗φ(ν)eν \varphi =\sum_{\nu\in\mathfrak{h}^*}\varphi (\nu )e^{\nu}

Let Z⟨P⟩\mathbf{Z}\langle P\rangle be the set of φ∈Zh∗\varphi \in \mathbf{Z}^{\mathfrak{h}^*} whose support is contained in a finite union of sets of the form ν−P+\nu -P_+, where ν∈h∗\nu \in \mathfrak{h}^*. Then Z[P]⊂Z⟨P⟩⊂Zh∗\mathbf{Z}[P]\subset \mathbf{Z}\langle P\rangle \subset \mathbf{Z}^{\mathfrak{h}^*}. Define on Z⟨P⟩\mathbf{Z}\langle P\rangle a ring structure extending that of Z[P]\mathbf{Z}[P] by putting, for φ,ψ∈Z⟨P⟩\varphi , \psi \in \mathbf{Z}\langle P\rangle and ν∈h∗\nu \in \mathfrak{h}^*,

(φψ)(ν)=∑μ∈h∗φ(μ)ψ(ν−μ) (\varphi \psi )(\nu ) =\sum_{\mu\in\mathfrak{h}^*}\varphi (\mu)\psi (\nu -\mu)

(the family (φ(μ)ψ(ν−μ))μ∈h∗(\varphi (\mu)\psi (\nu -\mu))_{\mu\in\mathfrak{h}^*} has finite support, in view of the condition satisfied by the supports of φ\varphi and ψ\psi ). If φ=∑νxνeν\varphi =\sum_{\nu}x_{\nu}e^{\nu} and ψ=∑νyνeν\psi =\sum_{\nu}y_{\nu}e^{\nu}, then φψ=∑ν,μxνyμeν+μ\varphi \psi =\sum_{\nu ,\mu}x_{\nu}y_\mu e^{\nu+\mu}.

Let ν∈h∗\nu \in \mathfrak{h}^*. A partition of ν\nu into positive roots is a family (nα)α∈R+(n_{\alpha})_{\alpha\in R_+}, where the nαn_{\alpha} are integers ≥0\geq 0 such that ν=∑α∈R+nαα\nu =\sum_{\alpha\in R_+}n_{\alpha}\alpha. We denote by P(ν)\mathfrak{P}(\nu ) the number of partitions of ν\nu into positive roots. We have

P(ν)>0⇐⇒ν∈Q+ \mathfrak{P}(\nu )>0\Leftarrow \Rightarrow \nu \in Q_+

In this paragraph, we denote by K the following element of Z⟨P⟩:\mathbf{Z}\langle P\rangle :

K=∑γ∈Q+P(γ)e−γ K =\sum_{\gamma\in Q_+}\mathfrak{P}(\gamma )e^{-\gamma}

Now recall (Chap. VI, §3, no. 3, Prop. 2) that

d=∏α∈R+(eα/2−e−α/2)=∑w∈Wε(w)ewρ d=\prod_{\alpha\in R_+}(e^{\alpha /2}-e^{-\alpha /2}) =\sum_{w\in W}\varepsilon (w)e^{w\rho}

is an anti-invariant element of Z[P]\mathbf{Z}[P].

Lemma 1 015T

In the ring Z⟨P⟩\mathbf{Z}\langle P\rangle, we have K.∏α∈R+(1−e−α)=Ke−ρd=1K.\prod_{\alpha\in R_+}(1-e^{-\alpha}) = Ke^{-\rho}d= 1.

Indeed,

K=∏α∈R+(e0+e−α+e−2α+⋯ ) K =\prod_{\alpha\in R_+}(e^0+e^{-\alpha}+e^{-2\alpha}+\cdots )

so

Ke−ρd=∏α∈R+(1+e−α+e−2α+⋯ )∏α∈R+(1−e−α)=1 Ke^{-\rho}d=\prod_{\alpha\in R_+}(1 +e^{-\alpha}+e^{-2\alpha}+\cdots )\prod_{\alpha\in R_+}(1-e^{-\alpha}) = 1

Lemma 2 015U

Let λ∈h∗\lambda \in \mathfrak{h}^*. The module Z(λ)(Z(\lambda ) (§6, no. 3) admits a character that is an element of Z⟨P⟩\mathbf{Z}\langle P\rangle, and we have dd. ch Z(λ)=eλ+ρZ(\lambda ) =e^{\lambda+\rho}.

Let α1,...,αq\alpha_1, . . . , \alpha_q be distinct elements of R+R_+. The X−α1n1X−α2n2...X−αqnq⊗1X_{-\alpha_1}^{n_1}X_{-\alpha_2}^{n_2}. . . X_{-\alpha_q}^{n_q}\otimes 1 form a basis of Z(λ)(Z(\lambda ) (§6, Prop. 6 (iii)). For h∈hh\in \mathfrak{h}, we have

h.(X−α1n1X−α2n2...X−αqnq⊗1) h.(X_{-\alpha_1}^{n_1}X_{-\alpha_2}^{n_2}. . .X_{-\alpha_q}^{n_q}\otimes 1)
=[h,X−α1n1...X−αqnq]⊗1+(X−α1n1...X−αqnq)⊗h.1 = [h, X_{-\alpha_1}^{n_1}. . . X_{-\alpha_q}^{n_q}]\otimes 1 + (X_{-\alpha_1}^{n_1}. . . X_{-\alpha_q}^{n_q})\otimes h.1
=(λ−n1α1−⋯−nqαq)(h)(X−α1n1...X−αqnq⊗1) = (\lambda -n_1\alpha_1- \cdots -n_q\alpha_q)(h)(X_{-\alpha_1}^{n_1}. . . X_{-\alpha_q}^{n_q}\otimes 1)

Thus, the dimension of Z(λ)λ−μZ(\lambda )^{\lambda-\mu} is P(μ)\mathfrak{P}(\mu). This proves that ch Z(λ)Z(\lambda ) is defined, is an element of Z⟨P⟩\mathbf{Z}\langle P\rangle, and that

ch Z(λ)=∑μP(μ)eλ−μ=KeλZ(\lambda ) =\sum_\mu\mathfrak{P}(\mu)e^{\lambda-\mu}= Ke^{\lambda}.

It now suffices to apply Lemma 1.

Lemma 3 015V

Let M be a g\mathfrak{g}-module which admits a character ch(M) whose support is contained in a finite union of the sets μ−P+\mu-P_+. Let U be the enveloping algebra of g\mathfrak{g}, Z the centre of U,λ0∈h∗,\lambda_0\in \mathfrak{h}^*, and χλ0\chi_{\lambda_0} the corresponding homomorphism from Z to k(k(§8, Cor. 1 of Th. 2). Assume that, for all z∈Z,zMz\in Z,z_M is the homothety with ratio χλ0(z)\chi_{\lambda_0}(z). Let DMD_M be the set of λ∈W(λ0+ρ)−ρ\lambda \in W(\lambda_0+\rho )-\rho such that λ+Q+\lambda + Q_+ meets Supp(ch M). Then ch(M) is a Z\mathbf{Z}-linear combination of the ch Z(λ)Z(\lambda ) for λ∈DM\lambda \in D_M.

If Supp(ch M) is empty, the lemma is clear. Assume that Supp(ch MM)≠∅\not=\emptyset. Let λ\lambda be a maximal element of this support, and put dim Mλ=mM^{\lambda}=m. There exists a g\mathfrak{g}-homomorphism φ\varphi from (Z(λ))m(Z(\lambda ))^m to M which maps (Z(λ)λ)m(Z(\lambda )^{\lambda})^m bijectively onto Mλ(M^{\lambda}(§6, no. 3, Prop. 6 (i)). Thus, the central character of Z(λ)Z(\lambda ) is χλ0\chi_{\lambda_0}, so λ∈W(λ0+ρ)−ρ(\lambda \in W(\lambda_0+\rho )-\rho (§8, no. 5, Cor. 1 of Th. 2). This proves that DM≠∅D_M\not=\emptyset, and allows us to argue by induction on Card DMD_M. Let L and N be the kernel and cokernel of φ\varphi. Then we have an exact sequence of g\mathfrak{g}-homomorphisms:

0→L→(Z(λ))m→M→N→0 0\rightarrow L\rightarrow (Z(\lambda ))^m\rightarrow M\rightarrow N\rightarrow 0

so

ch(M) =−=-ch(L) +m+m ch Z(λ)+Z(\lambda ) + 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+\mu-P_+. For z∈Z,zLz\in Z,z_L and zNz_N are homotheties with ratio χλ0(z)\chi_{\lambda_0}(z). Clearly, DN⊂DMD_N\subset D_M. On the other hand, (λ+Q+)∩(\lambda + Q_+)\capSupp(ch MM) ={λ}=\{\lambda \}, and λ∉\lambda \notin Supp(ch N), so λ∉DN\lambda \notin D_N and

Card DN<D_N< Card DMD_M.

On the other hand, L is a submodule of (Z(λ))m(Z(\lambda ))^m; if λ′∈DL\lambda '\in D_L, then λ′+Q+\lambda '+ Q_+ meets Supp(ch LL)⊂\subset Supp ch Z(λ)Z(\lambda ), so λ∈λ′+Q+(\lambda \in \lambda '+ Q_+(§6, no. 1, Prop. 1 (ii)); it follows that DL⊂DMD_L\subset D_M. Since L∩(Z(λ)λ)m=0L\cap (Z(\lambda )^{\lambda})^m= 0, we have λ∉DL\lambda \notin D_L, so

Card DL<D_L< Card DMD_M.

It now suffices to apply the induction hypothesis.

Theorem 1 (Character Formula of H. Weyl) 015W

Let M be a finite dimensional simple g\mathfrak{g}-module, and λ\lambda its highest weight. Then

(∑w∈Wε(w)ewρ)(\sum_{w\in W}\varepsilon (w)e^{w\rho}).ch M=∑w∈Wε(w)ew(λ+ρ)M =\sum_{w\in W}\varepsilon (w)e^{w(\lambda+\rho)}.

With the notations of Lemma 3, the central character of M is χλ(\chi_{\lambda}(§6, no. 4, Prop. 7). Hence, by Lemmas 2 and 3,d3,d.ch M is a Z\mathbf{Z}-linear combination of the eμ+ρe^{\mu+\rho} such that

μ+ρ∈W(λ+ρ) \mu+\rho \in W(\lambda +\rho )

On the other hand, by §7, no. 7, Lemma 7,d7,d.ch M is anti-invariant, and its unique maximal term is eλ+ρe^{\lambda+\rho}, hence the theorem.

Example 015X

Take g=sl(2,k),h=kH\mathfrak{g}=\mathfrak{s}\mathfrak{l}(2, k),\mathfrak{h}=kH. Let α\alpha be the root of (g,h)(\mathfrak{g},\mathfrak{h}) such that α(H)=2\alpha (H) = 2. The g\mathfrak{g}-module V(m)V(m) has highest weight (m/2)α(m/2)\alpha. Hence

ch(V(mm)) =(e(m/2)α+21α−e−(m/2)α−21α)/(e21α−e−21α)= (e^{(m/2)\alpha+^1_2\alpha}-e^{-(m/2)\alpha-^1_2\alpha})/(e^{^1_2\alpha}-e^{-^1_2\alpha})

=e−(m/2)α.(e(m+1)α−1)/(eα−1) =e^{-(m/2)\alpha}.(e^{(m+1)\alpha}-1)/(e^{\alpha}-1)
=e−(m/2)α(emα+e(m−1)α+⋯+1) =e^{-(m/2)\alpha}(e^{m\alpha}+e^{(m-1)\alpha}+\cdots + 1)
=e(m/2)α+e(m−2)α/2+⋯+e−(m/2)α =e^{(m/2)\alpha}+e^{(m-2)\alpha /2}+\cdots +e^{-(m/2)\alpha}

which also follows easily from §1, no. 2, Prop. 2.

2. Dimensions of simple g\mathfrak{g}-modules

If μ∈h∗\mu\in \mathfrak{h}^*, put J(eμ)=∑w∈Wε(w)ewμJ(e^\mu) =\sum_{w\in W}\varepsilon (w)e^{w\mu}, cf. Chap. VI, §3, no. 3.

Theorem 2 015Y

Let E be a finite dimensional simple g\mathfrak{g}-module, λ\lambda its highest weight and (⋅∣⋅)(\cdot | \cdot ) a W-invariant non-degenerate positive symmetric bilinear form on h∗\mathfrak{h}^*. Then:

∏⟨λ+ρ,Hα⟩∏((λ∣α)) \prod\langle \lambda +\rho , H_{\alpha}\rangle \prod((\lambda |\alpha ))

dim E = = 1 +.

α∈R+⟨ρ,Hα⟩α∈R+(ρ∣α)‾ _{\alpha\in R_+}\langle \rho , H_{\alpha}\rangle_{\alpha\in R_+}\overline{(\rho|\alpha)}

Let T be an indeterminate. For all ν∈P\nu \in P, denote by fνf_{\nu} the homomorphism from Z[P]\mathbf{Z}[P] to R[[T]]\mathbf{R}[[T]] that takes eμe^\mu to e(ν∣μ)Te^{(\nu|\mu)T} for all μ∈P\mu\in P. Then dim E is the constant term of the series fνf_{\nu}(ch E).

For all μ,ν∈P\mu, \nu \in P, we have

fν(J(eμ))=∑w∈Wε(w)e(ν∣wμ)T f_{\nu}(J(e^\mu)) =\sum_{w\in W}\varepsilon (w)e^{(\nu|w\mu)T}
=∑w∈Wε(w)e(w−1ν∣μ)T=fμ(J(eν)) =\sum_{w\in W}\varepsilon (w)e^{(w^{-1}\nu|\mu)T}=f_\mu(J(e^{\nu}))

In particular, in view of Chap. VI, §3, no. 3, formula (3),

fρ(J(eμ))=fμ(J(eρ))=e(μ∣ρ)T∏α∈R+(1−e−(μ∣α)T) f_{\rho}(J(e^\mu)) =f_\mu(J(e^{\rho})) =e^{(\mu|\rho)T}\prod_{\alpha\in R_+}(1-e^{-(\mu|\alpha)T})

Hence, setting Card(R+_+) =N= N,

fρ(J(eμ))≡TN∏α∈R(μ∣α)f_{\rho}(J(e^\mu))\equiv T^N\prod_{\alpha\in R}(\mu|\alpha ) (mod TN+1R[[T]]T^{N+1}\mathbf{R}[[T]]).

The equality J(eλ+ρ)=J(e^{\lambda+\rho}) = ch(E).J(eρ).J(e^{\rho}) (Th. 1) thus implies that

TN∏α∈R+(λ+ρ∣α)≡fρT^N\prod_{\alpha\in R_+}(\lambda +\rho |\alpha )\equiv f_{\rho}(ch EE).TN∏α∈R+(ρ∣α).T^N\prod_{\alpha\in R_+}(\rho |\alpha ) (mod TN+1R[[T]]T^{N+1}\mathbf{R}[[T]])

so

dim E=((∏α∈R+(λ+ρ∣α))/((∏α∈R+(ρ∣α))=∏α∈R+(1+(λ∣α)(ρ∣α))E =((\prod_{\alpha\in R_+}(\lambda +\rho |\alpha ))/((\prod_{\alpha\in R_+}(\rho |\alpha ))=\prod_{\alpha\in R_+}(1 +\frac{(\lambda|\alpha)}{(\rho|\alpha)}).

Now, if α∈R+,α\alpha \in R_+,\alpha can be identified with an element of hR\mathfrak{h}_{\mathbf{R}} proportional to HαH_{\alpha}, so

(λ+ρ∣α)/(ρ∣α)=⟨λ+ρ,Hα⟩/⟨ρ,Hα⟩ (\lambda +\rho |\alpha )/(\rho |\alpha ) =\langle \lambda +\rho , H_{\alpha}\rangle /\langle \rho , H_{\alpha}\rangle

Example 1 015Z

In the Example of no. 1, we find that

dim V(m)=(m2α+α2)(Hα)/α2(Hα)=m+1V(m) =(\frac{m}{2}\alpha +\frac{\alpha}{2})(H_{\alpha})/\frac{\alpha}{2}(H_{\alpha}) =m+ 1,

which we knew in §1.

Example 2 0160

Take g\mathfrak{g} to be the splittable simple Lie algebra of type G2G_2 and adopt the notations of Chap. VI, Plate IX. Give hR∗\mathfrak{h}^*_{\mathbf{R}} the W-invariant positive symmetric form (⋅∣⋅)(\cdot | \cdot ) such that (α1∣α1)=1(\alpha_1|\alpha_1) = 1. Then ρ=ϖ1+ϖ2\rho =\varpi_1+\varpi_2 and

(ϖ1∣α1)=12,(ϖ1∣α2)=0,(ϖ1∣α2+α1)=12 (\varpi_1|\alpha_1) =\frac{1}{2},(\varpi_1|\alpha_2) = 0,(\varpi_1|\alpha_2+\alpha_1) =\frac{1}{2}
(ϖ1∣α2+2α1)=1,(ϖ1∣α2+3α1)=32,(ϖ1∣2α2+3α1)=32 (\varpi_1|\alpha_2+ 2\alpha_1) = 1,(\varpi_1|\alpha_2+ 3\alpha_1) =\frac{3}{2},(\varpi_1|2\alpha_2+ 3\alpha_1) =\frac{3}{2}
(ϖ2∣α1)=0,(ϖ2∣α2)=32,(ϖ2∣α2+α1)=32 (\varpi_2|\alpha_1) = 0,(\varpi_2|\alpha_2) =\frac{3}{2},(\varpi_2|\alpha_2+\alpha_1) =\frac{3}{2}
(ϖ2∣α2+2α1)=32,(ϖ2∣α2+3α1)=32,(ϖ2∣2α2+3α1)=3 (\varpi_2|\alpha_2+ 2\alpha_1) =\frac{3}{2},(\varpi_2|\alpha_2+ 3\alpha_1) =\frac{3}{2},(\varpi_2|2\alpha_2+ 3\alpha_1) = 3

Thus, if n1,n2n_1, n_2 are integers ≥0\geq 0, the dimension of the simple representation of highest weight n1ϖ1+n2ϖ2n_1\varpi_1+n_2\varpi_2 is

(1+n1/212‾)((1+3n2/232‾)((1+n1/2+3n2/212‾+32)((1+n1+3n2/21+32‾) (1 +\frac{n_1/2}{1\overline{2}})((1 +\frac{3n_2/2}{3\overline{2}})((1 +\frac{n_1/2 + 3n_2/2}{_{1\overline{2}} + \frac{3}{2}})((1 +\frac{n_1 + 3n_2/2}{1 +^{3\overline{2}}})
×(1+3n1/2+3n2/232‾+32)((1+3n1/322+3+3n2) \times (1 +\frac{3n_1/2 + 3n_2/2}{_{3\overline{2}} + \frac{3}{2}})((1 +3n_1\frac{/_3}{2}2 + 3+ 3n_2)
=(1+n1)(1+n2)(1+n1+3n24)((1+2n1+3n25)((1+n1+n22) = (1 +n_1)(1 +n_2)(1 +\frac{n_1 + 3n_2}{4})((1 +\frac{2n_1 + 3n_2}{5})((1 +\frac{n_1 + n_2}{2})
×(1+n1+2n23) \times (1 +\frac{n_1 + 2n_2}{3})
(1+n1)(1+n2)(2+n1+n2)(3+n1+2n2)(4+n1+3n2)(5+2n1+3n2) (1+n_1)(1+n_2)(2+n_1+n_2)(3+n_1+2n_2)(4+n_1+3n_2)(5+2n_1+3n_2)

=.

5!

In particular, the fundamental representation of highest weight ϖ1\varpi_1 (resp. ϖ2\varpi_2) is of dimension 7 (resp. 14).

3. Multiplicities of weights of simple g\mathfrak{g}-modules

Proposition 1 0161

Let ω∈P++\omega \in P_{++}. For all λ∈P\lambda \in P, the multiplicity of λ\lambda in E(ω)E(\omega ) is

mλ=∑w∈Wε(w)P(w(ω+ρ)−(λ+ρ)) m_{\lambda}=\sum_{w\in W}\varepsilon (w)\mathfrak{P}(w(\omega +\rho )-(\lambda +\rho ))

By Th. 1 and Lemma 1,

ch E(ω)=Ke−ρdE(\omega ) = Ke^{-\rho}d ch E(ω)=Ke−ρ∑w∈Wε(w)ew(ω+ρ)E(\omega ) = Ke^{-\rho}\sum_{w\in W}\varepsilon (w)e^{w(\omega+\rho)}

so

ch E(ω)=∑w∈W,γ∈Q+ε(w)P(γ)e−ρ+w(ω+ρ)−γE(\omega ) =\sum_{w\in W,\gamma\in Q_+}\varepsilon (w)\mathfrak{P}(\gamma )e^{-\rho+w(\omega+\rho)-\gamma}

and

mλ=∑ε(w)P(γ) m_{\lambda}=\sum\varepsilon (w)\mathfrak{P}(\gamma )
w∈W,γ∈Q+,γ=−λ−ρ+w(ω+ρ)w\in W,\gamma \in Q_+,\gamma =-\lambda -\rho +w(\omega +\rho )

Corollary 0162

If λ\lambda is a weight of E(ω)E(\omega ) distinct from ω\omega,

mλ=−∑w∈W,w≠1ε(w)mλ+ρ−wρ m_{\lambda}=-\sum_{w\in W,w\not=1}\varepsilon (w)m_{\lambda+\rho-w\rho}

Apply Prop. 1 with ω=0\omega = 0. If μ∈P\mu\in P-- {0}\{0\}, we find that

0=∑w∈Wε(w)P(wρ+μ−ρ) 0 =\sum_{w\in W}\varepsilon (w)\mathfrak{P}(w\rho +\mu-\rho )

hence

P(μ)=−∑w∈W,w≠1ε(w)P(μ+wρ−ρ)(1) \mathfrak{P}(\mu) =-\sum_{w\in W,w\not=1}\varepsilon (w)\mathfrak{P}(\mu+w\rho -\rho ) \tag{1}

Prop. 1 also gives

mλ=−∑w∈Wε(w)∑w′∈W,w′≠1ε(w′)P(w(ω+ρ)−(λ+ρ)+w′ρ−ρ) m_{\lambda}=-\sum_{w\in W}\varepsilon (w)\sum_{w'\in W,w'\not=1}\varepsilon (w')\mathfrak{P}(w(\omega +\rho )-(\lambda +\rho ) +w'\rho -\rho )

since w(ω+ρ)≠λ+ρw(\omega +\rho )\not=\lambda +\rho for all w∈W(w\in W (§7, Prop. 5 (iii)). Hence,

mλ=−∑w′∈W,w′≠1ε(w′)∑w∈Wε(w)P(w(ω+ρ)−(λ+ρ−w′ρ+ρ)) m_{\lambda}=-\sum_{w'\in W,w'\not=1}\varepsilon (w')\sum_{w\in W}\varepsilon (w)\mathfrak{P}(w(\omega +\rho )-(\lambda +\rho -w'\rho +\rho ))

=−∑w′∈W,w′≠1ε(w′)mλ+ρ−w′ρ=-\sum_{w'\in W,w'\not=1}\varepsilon (w')m_{\lambda+\rho-w'\rho} (Prop.1.1).

4. Decomposition of tensor products of simple g\mathfrak{g}-modules

Proposition 2 0163

Let λ,μ∈P++\lambda , \mu\in P_{++}. In R(g)\mathscr{R}(\mathfrak{g}), we have

[λ].[μ]=∑ν∈P++m(λ,μ,ν)[ν] [\lambda ].[\mu] =\sum_{\nu\in P_{++}}m(\lambda , \mu, \nu )[\nu ]

with

m(λ,μ,ν)=∑w,w′∈Wε(ww′)P(w(λ+ρ)+w′(μ+ρ)−(ν+2ρ)) m(\lambda , \mu, \nu ) =\sum_{w,w'\in W}\varepsilon (ww')\mathfrak{P}(w(\lambda +\rho ) +w'(\mu+\rho )-(\nu + 2\rho ))

Let E,FE,F be finite dimensional simple g\mathfrak{g}-modules of highest weights λ,μ\lambda , \mu. Let lνl_{\nu} be the length of the isotypical component of E⊗FE\otimes F of highest weight ν\nu. It suffices to show that

lν=∑w,w′∈Wε(ww′)P(w(λ+ρ)+w′(μ+ρ)−(ν+2ρ))(2) l_{\nu}=\sum_{w,w'\in W}\varepsilon (ww')\mathfrak{P}(w(\lambda +\rho ) +w'(\mu+\rho )-(\nu + 2\rho )) \tag{2}

Put c1=c_1= ch(E) =∑σ∈Pmσeσ,c2==\sum_{\sigma\in P}m_{\sigma}e^{\sigma},c_2= ch(F), and d=J(eρ)d= J(e^{\rho}), where J is defined as in no. 2. We have ∑ξ∈P++lξ\sum_{\xi\in P_{++}}l_{\xi}ch[ξ]=\xi ] = ch(E ⊗F\otimes F) =c1c2=c_1c_2

so, after multiplying by dd and using Th. 1,

∑ξ∈P++lξJ(eξ+ρ)=c1J(eμ+ρ)=(∑σ∈Pmσeσ)((∑w∈Wε(w)ew(μ+ρ))(3) \sum_{\xi\in P_{++}}l_{\xi}J(e^{\xi+\rho}) =c_1J(e^{\mu+\rho}) =(\sum_{\sigma\in P}m_{\sigma}e^{\sigma})((\sum_{w\in W}\varepsilon (w)e^{w(\mu+\rho)}) \tag{3}
=∑τ∈P(∑w∈Wε(w)mτ+ρ−w(μ+ρ))eτ+ρ =\sum_{\tau\in P}(\sum_{w\in W}\varepsilon (w)m_{\tau+\rho-w(\mu+\rho)})e^{\tau+\rho}

Now, if ξ∈P++,ξ+ρ\xi \in P_{++},\xi +\rho belongs to the chamber defined by B (Chap. VI, §1, no. 10); thus, for all w∈Ww\in W distinct from 1, we have w(ξ+ρ)∉P++w(\xi +\rho )\notin P_{++}. Consequently, the coefficient of eν+ρe^{\nu+\rho} in ∑ξ∈P++lξJ(eξ+ρ)\sum_{\xi\in P_{++}}l_{\xi}J(e^{\xi+\rho}) is equal to lνl_{\nu}. In view of (3), we obtain

lν=∑w∈Wε(w)mν+ρ−w(μ+ρ) l_{\nu}=\sum_{w\in W}\varepsilon (w)m_{\nu+\rho-w(\mu+\rho)}

that is, by Prop. 1,

lν=∑w,w′∈Wε(w)ε(w′)P(w′(λ+ρ)−(ν+ρ−w(μ+ρ)+ρ)) l_{\nu}=\sum_{w,w'\in W}\varepsilon (w)\varepsilon (w')\mathfrak{P}(w'(\lambda +\rho )-(\nu +\rho -w(\mu+\rho ) +\rho ))

which proves (2).

Example 0164

We return to the Example of no. 1. Let λ=(n/2)α,μ=(p/2)α\lambda = (n/2)\alpha , \mu= (p/2)\alpha, ν=(q/2)α\nu = (q/2)\alpha with n≥pn\geq p. We have

m(λ,μ,ν)=P(n2α+α2+p2α+α2−q2α−α) m(\lambda , \mu, \nu ) =\mathfrak{P}(\frac{n}{2}\alpha +\frac{\alpha}{2}+\frac{p}{2}\alpha +\frac{\alpha}{2}-\frac{q}{2}\alpha -\alpha )
−P(n2α+α2−p2α−α2−q2α−α) -\mathfrak{P}(\frac{n}{2}\alpha +\frac{\alpha}{2}-\frac{p}{2}\alpha -\frac{\alpha}{2}-\frac{q}{2}\alpha -\alpha )
−P(−n2α−α2+p2α+α2−q2α−α) -\mathfrak{P}(-\frac{n}{2}\alpha -\frac{\alpha}{2}+\frac{p}{2}\alpha +\frac{\alpha}{2}-\frac{q}{2}\alpha -\alpha )
+P(−n2α−α2−p2α−α2−q2α−α) +\mathfrak{P}(-\frac{n}{2}\alpha -\frac{\alpha}{2}-\frac{p}{2}\alpha -\frac{\alpha}{2}-\frac{q}{2}\alpha -\alpha )
=P(n+p−q2α)−P(n−p−q−22α) =\mathfrak{P}(\frac{n + p-q}{2}\alpha )-\mathfrak{P}(\frac{n-p-q- 2}{2}\alpha )

This is zero if n+p+qn+p+q is not divisible by 2, or if q≥n+pq\geq n+p. If

q=n+p−2r q=n+p-2r

with rr an integer ≥0\geq 0, we have

m(λ,μ,ν)=P(rα)−P((r−p−1)α) m(\lambda , \mu, \nu ) =\mathfrak{P}(r\alpha )-\mathfrak{P}((r-p-1)\alpha )

hence m(λ,μ,ν)=1m(\lambda , \mu, \nu ) = 1 if r≤pr\leq p and m(λ,μ,ν)=0m(\lambda , \mu, \nu ) = 0 if r>pr > p. Finally, the g\mathfrak{g}-module V(n)⊗V(p)V(n)\otimes V(p) is isomorphic to

V(n+p)⊕V(n+p−2)⊕V(n+p−4)⊕⋯⊕V(n−p) V(n+p)\oplus V(n+p-2)\oplus V(n+p-4)\oplus \cdots \oplus V(n-p)

(Clebsch-Gordan formula).

Exercises

All the g\mathfrak{g}-modules considered are assumed to be finite dimensional.

See the exercises for § 9.

Transcribed from the printed volume. Not translated.