Bourbaki

§ 1. The Lie algebra sl\mathfrak{s}\mathfrak{l}(2,k\boldsymbol{, k}) and its representations

1. Canonical basis of sl\mathfrak{s}\mathfrak{l}(2,k\boldsymbol{, k})

Lemma 1 00XS

Let A be an associative algebra over k,Hk,H and XX elements of A such that [H,X]=2X[H, X] = 2X.

(i) [H,Xn]=2nXn[H, X^n] = 2nX^n for any integer n≥0n\geq 0.

(ii) If ZZ is an element of A such that [Z,X]=H[Z, X] =H, then, for any integer n>0n >0,

[Z,Xn]=nXn−1(H+n−1)=n(H−n+1)Xn−1 [Z, X^n] =nX^{n-1}(H+n-1) =n(H-n+ 1)X^{n-1}

The map T→[H,T]T \rightarrow [H, T] from A to A is a derivation, which implies (i). With the assumptions in (ii),

[Z,Xn]=∑i+j=n−1XiHXj [Z, X^n] =\sum_{i+j=n-1}X^iHX^j
=∑i+j=n−1(XiXjH+Xi2jXj) =\sum_{i+j=n-1}(X^iX^jH+X^i2jX^j)
=nXn−1H+2Xn−1n(n−1)2 =nX^{n-1}H+ 2X^{n-1}\frac{n(n- 1)}{2}
=nXn−1(H+n−1) =nX^{n-1}(H+n-1)

On the other hand, Xn−1(H+n−1)=(H−n+1)Xn−1X^{n-1}(H+n-1) = (H-n+ 1)X^{n-1} by (i). Q.E.D.

Recall that we denote by sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) the Lie algebra consisting of the square matrices of order 2, trace zero, and with entries in kk. This Lie algebra is simple of dimension 3 (Chap. I, §6, no. 7, Example). The canonical basis of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) is the basis (X+,X−,H)(X_+, X_-, H), where

(01)((01)( 0 0)(10)(1 0 ))

X+=X_+= 0 0 X−=−1X_-=-1 0 H=H= 0 −1-1.

We have

[H,X+]=2X+[H,X−]=−2X−[X+,X−]=−H(1) [H, X_+] = 2X_+[H, X_-] =-2X_-[X_+, X_-] =-H \tag{1}

Since the identity representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) is injective, HH is a semi-simple element of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) and X+,X−X_+, X_- are nilpotent elements of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) (Chap. I, §6, no. 3, Th. 3). By Chap. VII, §2, no. 1, Example 4,kH4,kH is a Cartan subalgebra of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k). The map U→−tUU \rightarrow -^tU is an involutive automorphism of the Lie algebra sl(2,k)\mathfrak{s}\mathfrak{l}(2, k), called the canonical involution of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k); it transforms (X+,X−,H)(X_+, X_-, H) into (X−,X+,−H)(X_-, X_+,-H).

Lemma 2 00XT

In the enveloping algebra of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k),

[H,X+n]=2nX+n[H,X−n]=−2nX−n [H, X_+^n] = 2nX_+^n[H, X_-^n] =-2nX_-^n

for any integer n≥0n\geq 0, and

[X−,X+n]=nX+n−1(H+n−1)=n(H−n+1)X+n−1 [X_-, X_+^n] =nX_+^{n-1}(H+n-1) =n(H-n+ 1)X_+^{n-1}
[X+,X−n]=nX−n−1(−H+n−1)=n(−H−n+1)X−n−1 [X_+, X_-^n] =nX_-^{n-1}(-H+n-1) =n(-H-n+ 1)X_-^{n-1}

if n>0n >0.

The first and third relations follow from Lemma 1. The others can be deduced from them by using the canonical involution of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k).

2. Primitive elements of sl\mathfrak{s}\mathfrak{l}(2,k\boldsymbol{, k})-modules

Let E be an sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module. If A∈sl(2,k)A\in \mathfrak{s}\mathfrak{l}(2, k) and x∈Ex\in E, we shall often write AxAx instead of AExA_Ex. Let λ∈k\lambda \in k. If Hx=λxHx=\lambda x we say, by abuse of language, that xx is an element of E of weight λ\lambda, or that λ\lambda is the weight of xx. If E is finite dimensional, HEH_E is semi-simple, so the set of elements of weight λ\lambda is the primary subspace of E relative to HEH_E and λ\lambda (cf. Chap. VII, §1, no. 1).

Lemma 3 00XU

If xx is an element of weight λ\lambda, then X+xX_+x is an element of weight λ+2\lambda + 2 and X−xX_-x is an element of weight λ−2\lambda -2.

Indeed, HX+x=[H,X+]x+X+Hx=2X+x+X+λx=(λ+2)X+xHX_+x= [H, X_+]x+X_+Hx= 2X_+x+X_+\lambda x= (\lambda + 2)X_+x, and similarly HX−x=(λ−2)X−xHX_-x= (\lambda -2)X_-x (cf. also Chap. VII, §1, no. 3, Prop. 10 (ii)).

Definition 1 00XV

Let E be an sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module. An element of E is said to be primitive if it is a non-zero eigenvector of HEH_E and belongs to the kernel of X+EX_{+E}.

A non-zero element ee of E is primitive if and only if keke is stable under the operation of kH+kX+kH+kX_+; this follows for example from Lemma 3.

Examples The element X+X_+ is primitive of weight 2 for the adjoint representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k). The element (1,0)(1,0) of k2k^2 is primitive of weight 1 for the identity representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) on k2k^2.

Lemma 4 00XW

Let E be a non-zero finite dimensional sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module. Then E has primitive elements.

Since X+X_+ is a nilpotent element of sl(2,k),X+E\mathfrak{s}\mathfrak{l}(2, k),X_{+E} is nilpotent. Assume that X+Em−1≠0X_{+E}^{m-1}\not= 0 and X+EmX_{+E}^m = 0. By Lemma 2,

m(HE−m+1)X+Em−1=[X−E,X+Em]=0 m(H_E-m+ 1)X_{+E}^{m-1}= [X_{-E}, X_{+E}^m] = 0

and hence the elements of X+m−1(E)X_+^{m-1}(E)-- {0}\{0\} are primitive.

Proposition 1 00XX

Let E be an sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module, and ee a primitive element of E of weight λ\lambda. Put en=(−1)nnX−nee_n=\frac{(-1)^n}{n}X_-^ne for n≥0n\geq 0, and e−1=0e_{-1}= 0. Then

Hen=(λ−2n)en He_n= (\lambda -2n)e_n
X−en=−(n+1)en+1(2) X_-e_n=-(n+ 1)e_{n+1} \tag{2}
X+en=(λ−n+1)en−1 X_+e_n= (\lambda -n+ 1)e_{n-1}

The first formula follows from Lemma 3, and the second from the definition of the ene_n. We prove the third by induction on nn. It is satisfied for n=0n= 0 since e−1=0e_{-1}= 0. If n>0n >0,

nX+en=−X+X−en−1=−[X+,X−]en−1−X−X+en−1 nX_+e_n=-X_+X_-e_{n-1}=-[X_+, X_-]e_{n-1}-X_-X_+e_{n-1}
=Hen−1−X−(λ−n+2)en−2 =He_{n-1}-X_-(\lambda -n+ 2)e_{n-2}
=(λ−2n+2+(n−1)(λ−n+2))en−1 = (\lambda -2n+ 2 + (n-1)(\lambda -n+ 2))e_{n-1}
=n(λ−n+1)en−1 =n(\lambda -n+ 1)e_{n-1}

Corollary 00XY

The submodule of E generated by ee is the vector subspace generated by the ene_n.

This follows from the formulas (2).

The integers n≥0n\geq 0 such that en≠0e_n\not= 0 constitute an interval in N\mathbf{N}, and the corresponding elements ene_n form a basis over kk of the submodule generated by ee (indeed, they are linearly independent because they are non-zero elements of distinct weights). This basis will be said to be associated to the primitive element ee.

Proposition 2 00XZ

If the submodule V of E generated by the primitive element ee is finite dimensional, then:

(i) the weight λ\lambda of ee is integral and equal to dim V−1V-1;

(ii) (e0,e1,...,eλ)(e_0, e_1, . . . , e_{\lambda}) is a basis of V, and en=0e_n= 0 for n>λn > \lambda;

(iii) the eigenvalues of HVH_V are λ,λ−2,λ−4,...,−λ\lambda , \lambda -2, \lambda -4, . . . ,-\lambda; they are all of multiplicity 1;

(iv) every primitive element of V is proportional to ee;

(v) the commutant of the module V is reduced to the scalars; in particular, V is absolutely simple.

Let mm be the largest integer such that em≠0e_m\not= 0. Then 0=X+em+1=0 =X_+e_{m+1}= (λ−m)em(\lambda -m)e_m, so λ=m\lambda =m; since (e0,e1,...,em)(e_0, e_1, . . . , e_m) is a basis of V, this proves (i) and (ii). Assertion (iii) follows from the equality Hen=(λ−2n)enHe_n= (\lambda -2n)e_n. We have X+en≠0X_+e_n\not= 0 for 1≤n≤m1\leq n\leq m, hence (iv). Let cc be an element of the commutant of the module V. Then Hc(e)=cH(e)=λc(e)Hc(e) =cH(e) =\lambda c(e), so there exists μ∈k\mu\in k such that c(e)=μec(e) =\mu e; then

cX−qe=X−qce=μX−qe cX_-^qe=X_-^qce=\mu X_-^qe

for all q≥0q\geq 0, so c=μ.1c=\mu.1, proving (v).

Corollary 00Y0

Let E be a finite dimensional sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module.

(i) The endomorphism HEH_E is diagonalizable and its eigenvalues are rational integers.

(ii) For any p∈Zp\in \mathbf{Z}, let EpE_p be the eigenspace of HEH_E corresponding to the eigenvalue pp. Let ii be an integer ≥0\geq 0. The map X−Ei∣Ep:Ep→Ep−2iX_{-E}^i|E_p: E_p\rightarrow E_{p-2i} is injective for i≤pi\leq p, bijective for i=pi=p, and surjective for i≥pi\geq p. The map X+Ei∣E−p:E−p→E−p+2iX_{+E}^i|E_{-p}: E_{-p}\rightarrow E_{-p+2i} is injective for i≤pi\leq p, bijective for i=pi=p, and surjective for i≥pi\geq p.

(iii) The length of E is equal to dim KerX+EX_{+E} and to dim KerX−EX_{-E}.

(iv) Let E′E' (resp. E′′E'') be the sum of the EpE_p for pp even (resp. odd). Then E′E' (resp. E′′E'') is the sum of the simple submodules of E of odd (resp. even) dimension; and E=E′⊕E′′E = E'\oplus E''. The length of E′E' is dim E0E_0, and that of E′′E'' is dim E1E_1.

(v) KerX+E∩X_{+E}\cap ImX+E⊂∑p>0EpX_{+E}\subset \sum_{p>0}E_p and KerX−E∩X_{-E}\cap ImX−E⊂∑p<0EpX_{-E}\subset \sum_{p<0}E_p.

If E is simple, E is generated by a primitive element (Lemma 4), and it suffices to apply Propositions 1 and 2. The general case follows since every finite dimensional sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module is semi-simple.

3. The simple modules v(m\boldsymbol{m})

Let (u,v)(u, v) be the canonical basis of k2k^2. For the identity representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k),

X+u=0Hu=uX−u=−v X_+u= 0Hu=uX_-u=-v
X+v=uHv=−vX−v=0 X_+v=uHv=-vX_-v= 0

Consider the symmetric algebra S(k2)\mathbf{S}(k^2) of k2(k^2(Algebra, Chap. III, §6, no. 1, Def. 1). The elements of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) extend uniquely to derivations of S(k2)\mathbf{S}(k^2), giving S(k2)\mathbf{S}(k^2) the structure of an sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module (Chap. I, §3, no. 2). Let V(m)V(m) be the set of homogeneous elements of S(k2)\mathbf{S}(k^2) of degree mm. Then V(m)V(m) is an sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-submodule of S(k2)\mathbf{S}(k^2) of dimension m+1m+ 1, the mmth symmetric power of V(1)=k2V(1) =k^2 (Chap. III, Appendix). If m,nm, n are integers such that 0≤n≤m0\leq n\leq m, put

en(m)=(m)um−nvn∈V(m) e^{(m)}_n=(m)u^{m-n}v^n\in V(m)
n n

Proposition 3 00Y1

For any integer m≥0m\geq 0, V(m)V(m) is an absolutely simple sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module. In this module, e0(m)=ume^{(m)}_0=u^m is primitive of weight mm.

We have X+um=0X_+u^m= 0 and Hum=mumHu^m=mu^m, so umu^m is primitive of weight mm. The submodule of V(m)V(m) generated by umu^m is of dimension m+1m+ 1 (Prop. 2 (i)) and so is equal to V(m)V(m). By Prop. 2 (v), V(m)V(m) is absolutely simple.

Theorem 1 00Y2

Every simple sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module of finite dimension nn is isomorphic to V(n−1)V(n-1). Every finite dimensional sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module is a direct sum of submodules isomorphic to the modules V(m)V(m).

This follows from Lemma 4 and Prop. 1, 2 and 3.

Remark 1 00Y3

The adjoint representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) defines on sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) the structure of a simple sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module. This module is isomorphic to V(2) by an isomorphism that takes u2u^2 to X+,2uvX_+, 2uv to −H-H, and v2v^2 to X−X_-.

Remark 2 00Y4

For n≥0n\geq 0 and m>nm > n,

X−en(m)=−(m−n)(m)um−n−1vn+1=−(n+1)en+1(m) X_-e^{(m)}_n=-(m-n)(m)u^{m-n-1}v^{n+1}=-(n+ 1)e^{(m)}_{n+1}
n n

Hence, (e0(m),e1(m),...,em(m))(e_0^{(m)}, e_1^{(m)}, . . . , e_m^{(m)}) is the basis of V(m)V(m) associated to the primitive element e0(m)e_0^{(m)}.

Remark 3 00Y5

Let Φ\Phi be the bilinear form on V(m)V(m) such that

Φ(en(m),en′(m))=0\Phi (e^{(m)}_n, e^{(m)}_{n'}) = 0 if n+n′≠mn+n'\not=m

Φ(en(m),em−n(m))=(−1)n(m) \Phi (e^{(m)}_n, e^{(m)}_{m-n}) = (-1)^n(m)
n n

If x=au+bvx=au+bv and y=cu+dvy=cu+dv, then Φ(xm,ym)=(ad−bc)m\Phi (x^m, y^m) = (ad-bc)^m. It is now easy to check that Φ\Phi is invariant, and that Φ\Phi is symmetric for mm even, and alternating for mm odd.

Proposition 4 00Y6

Let E be a finite dimensional sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module, mm an integer ≥0\geq 0, PmP_m the set of primitive elements of weight mm. Let L be the vector space of homomorphisms from the sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module V(m)V(m) to the sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module E. The map f→f(um)f \rightarrow f(u^m) from L to E is linear, injective, and its image is Pm∪{0}P_m\cup \{0\}.

This map is clearly linear, and it is injective because umu^m generates the sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module V(m)V(m). If f∈Lf\in L,

X+(f(um))=f(X+um)=0,H(f(um))=f(Hum)=mf(um) X_+(f(u^m)) =f(X_+u^m) = 0,H(f(u^m)) =f(Hu^m) =mf(u^m)

so f(um)∈Pm∪{0}f(u^m)\in P_m\cup \{0\}. Let e∈Pme\in P_m, and V the submodule of E generated by ee. By Prop. 1, there exists an isomorphism from the module V(m)V(m) to the module V that takes umu^m to ee. Then L(um)=Pm∪{0}L(u^m) = P_m\cup \{0\}.

Corollary 00Y7

The isotypical component of E of type V(m)V(m) has length

dim(Pm∪{0}_m\cup \{0\}.

4. Linear representations of the group sl(2,k\boldsymbol{, k})

Recall (Algebra, Chap. III, §8, no. 9) that we denote by SL(2,k)\mathbf{S}\mathbf{L}(2, k) the group of square matrices of order 2 with coefficients in kk whose determinant is equal to 1. If x∈sl(2,k)x\in \mathfrak{s}\mathfrak{l}(2, k) is nilpotent, then x2=0(x^2= 0 (Algebra, Chap. VII, §5, Cor. 3 of Prop. 5) and ex=1+x∈SL(2,k)e^x= 1 +x\in \mathbf{S}\mathbf{L}(2, k). If E is a finite dimensional vector space and ρ\rho is a linear representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) on E, then ρ(x)\rho (x) is nilpotent and so eρ(x)e^{\rho(x)} is defined (Chap. I, §6, no. 3).

Definition 2 00Y8

Let E be a finite dimensional vector space, and ρ\rho (resp. π\pi ) a linear representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) (resp. SL(2,k)\mathbf{S}\mathbf{L}(2, k)) on E. Then ρ\rho and π\pi are said to be compatible if, for every nilpotent element xx of sl(2,k),π(ex)=eρ(x)\mathfrak{s}\mathfrak{l}(2, k),\pi (e^x) =e^{\rho(x)}.

In other words, ρ\rho and π\pi are compatible if, for every nilpotent element xx of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k), the restriction of ρ\rho to kxkx is compatible with the restriction of π\pi to the group 1+kx1 +kx (Chap. VII, §3, no. 1).

If ρ\rho and π\pi are compatible, so are the dual representations, the mmth tensor powers, and the mmth symmetric powers of ρ\rho and π\pi, respectively (Chap. VII, §5, no. 4, Lemma 1 (i) and (ii)). Similarly for the representations induced by ρ\rho and π\pi on a vector subspace stable under ρ\rho and π(\pi (loc. cit.).

In particular, the representation ρm\rho_m of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) on V(m)V(m) (no. 3) is compatible with the mmth symmetric power πm\pi_m of the identity representation π1\pi_1 of SL(2,k)\mathbf{S}\mathbf{L}(2, k). Putting en(m)=(nm)um−nvne^{(m)}_n=(^m_n)u^{m-n}v^n as above, we have

(m)(m)m−nn(m)(m)m-nn

πm(s)en\pi_m(s)e_n = (su)(sv)(su)(sv) (3)

n n

for s∈SL(2,k)s\in \mathbf{S}\mathbf{L}(2, k) and 0≤n≤m0\leq n\leq m.

Theorem 2 00Y9

Let ρ\rho be a linear representation of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) on a finite dimensional vector space E.

(i) There exists a unique linear representation π\pi of SL(2,k)\mathbf{S}\mathbf{L}(2, k) on E that is compatible with ρ\rho.

(ii) A vector subspace F of E is stable under π\pi if and only if it is stable under ρ\rho.

(iii) Let x∈Ex\in E. Then π(s)x=x\pi (s)x=x for all s∈SL(2,k)s\in \mathbf{S}\mathbf{L}(2, k) if and only if xx is invariant under ρ(\rho (that is, ρ(a)x=0\rho (a)x= 0 for all a∈sl(2,k))a\in \mathfrak{s}\mathfrak{l}(2, k)).

The existence of π\pi follows from the preceding and Th. 1. On the other hand, we know that the group SL(2,k)\mathbf{S}\mathbf{L}(2, k) is generated by the elements of the form

tX(1t)−tX−(10) _{tX}(1t)_{-tX_-}(10)

e+=ee^+=e =

0 1 tt 1

where t∈k(t\in k(Algebra, Chap. III, §8, no. 9, Prop. 17). This proves the uniqueness of π\pi.

Assertions (ii) and (iii) follow from what we have said, together with Chap. VII, §3, no. 1, Lemma 1 (i). Q.E.D.

Every finite dimensional sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module therefore has a unique SL(2,k)\mathbf{S}\mathbf{L}(2, k)-module structure, which is said to be associated to its sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module structure.

Remark 00YA

When kk is R\mathbf{R} or C\mathbf{C} or a complete non-discrete ultrametric field, sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) is the Lie algebra of SL(2,k)\mathbf{S}\mathbf{L}(2, k). Let ρ\rho and π\pi be as in Th. 2. The homomorphism π\pi is a homomorphism of Lie groups from SL(2,k)\mathbf{S}\mathbf{L}(2, k) to GL(E):\mathbf{G}\mathbf{L}(E): this is clear when E=V(m)E = V(m), and the general case follows, in view of Th. 1. By Chap. VII, §3, no. 1,ρ(X+)=L(π)(X+),ρ(X−)=L(π)(X−)1,\rho (X_+) = L(\pi )(X_+),\rho (X_-) = L(\pi )(X_-). Hence ρ=L(π)\rho = L(\pi ) (for a converse, see Exerc. 18).

Proposition 5 00YB

Let E, F be finite dimensional sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-modules, and let f∈f\in Homk(E,F)_k(E,F). The following conditions are equivalent:

(i) ff is a homomorphism of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-modules;

(ii) ff is a homomorphism of SL(2,k)\mathbf{S}\mathbf{L}(2, k)-modules.

Condition (i) means that ff is an invariant element of the sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module Homk(E,F)_k(E,F), and condition (ii) means that ff is an invariant element of the SL(2,k\mathbf{S}\mathbf{L}(2, k)-module Homk(E,F)_k(E,F). Since these module structures are associated by Chap. VII, §5, no. 4, Lemma 1 (iii), the proposition follows from Th. 2 (iii).

Definition 3 00YC

The adjoint representation of the group SL(2,k)\mathbf{S}\mathbf{L}(2, k) is the linear representation Ad of SL(2,k)\mathbf{S}\mathbf{L}(2, k) on sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) defined by

Ad(ss).a=sas−1.a=sas^{-1}

for all a∈sl(2,k)a\in \mathfrak{s}\mathfrak{l}(2, k) and all s∈SL(2,k)s\in \mathbf{S}\mathbf{L}(2, k). When kk is R\mathbf{R} or C\mathbf{C} or a complete non-discrete ultrametric field, we recover Def. 7 of Chap. III, §3, no. 12 (cf. loc. cit., Prop. 49).

By Chap. VII, §5, no. 4, Lemma 1 (i) and (ii), the adjoint representations of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k) and SL(2,k)\mathbf{S}\mathbf{L}(2, k) are compatible. By Chap. VII, §3, no. 1, Remark 2, Ad(SL(2,k)\mathbf{S}\mathbf{L}(2, k)) == Aute(sl(2,k))_e(\mathfrak{s}\mathfrak{l}(2, k)).

5. Some elements of sl(2,k\boldsymbol{, k})

For any t∈k∗t\in k^*, put

θ(t)=etX+et−1X−etX+ \theta (t) =e^{tX_+}e^{t^{-1}X_-}e^{tX_+}

(1t)(((1t)(( 1 0)((1t)0)((1t)

= 0 1 −t−1-t^{-1} 1 0 1

(( 0 t)

= −t−1-t^{-1} 0

=et−1X−etX+et−1X− =e^{t^{-1}X_-}e^{tX_+}e^{t^{-1}X_-}

With the notations of no. 3,

θ(t)u=−t−1vθ(t)v=tu \theta (t)u=-t^{-1}v\theta (t)v=tu

so

θ(t)en(m)=(−1)m−nt2n−mem−n(m)(4) \theta (t)e^{(m)}_n= (-1)^{m-n}t^{2n-m}e^{(m)}_{m-n} \tag{4}

Hence, the element θ(t)2=(−1\theta (t)^2=(-1 0 )) operates by (−1)m(-1)^m on V(m)V(m). If

0 −1-1

E is an odd-dimensional simple sl(2,k\mathfrak{s}\mathfrak{l}(2, k)-module, θ(t)E\theta (t)_E is thus an involutive automorphism of the vector space E. In particular, taking E to be the adjoint representation:

θ(t)EX+=t−2X−θ(t)EX−=t2X+θ(t)EH=−H(5) \theta (t)_EX_+=t^{-2}X_-\theta (t)_EX_-=t^2X_+\theta (t)_EH=-H \tag{5}

so that θ(1)E=θ(−1)E\theta (1)_E=\theta (-1)_E is the canonical involution of sl(2,k)\mathfrak{s}\mathfrak{l}(2, k).

For any t∈k∗t\in k^*, put

h(t)=(0tt−01)=θ(t)θ(−1) h(t) =(0tt^-0_1)=\theta (t)\theta (-1)

Then h(t)u=tu,h(t)v=t−1vh(t)u=tu,h(t)v=t^{-1}v, so

h(t)en(m)=tm−2nen(m)(6) h(t)e^{(m)}_n=t^{m-2n}e^{(m)}_n \tag{6}

Proposition 6 01L4

Let E be a finite dimensional sl(2,k)\mathfrak{s}\mathfrak{l}(2, k)-module, and t∈k∗t\in k^*. Let EpE_p be the set of elements of E of weight pp.

(i) θ(t)E∣Ep\theta (t)_E|E_p is a bijection from EpE_p to E−pE_{-p}.

(ii) h(t)E∣Eph(t)_E|E_p is the homothety with ratio tpt^p on EpE_p.

If E=V(n)E = V(n), the proposition follows from formulas (4) and (6). The general case follows from Th. 1.

Corollary 00YD

Let E=E′⊕E′′E = E'\oplus E'' be the decomposition of E defined in the Cor. of Prop. 2. The element (−10)(-10) of SL(2,k)\mathbf{S}\mathbf{L}(2, k) operates by +1 on E′E'

0 −1-1

and by −1-1 on E′′E''.

This follows from (ii), applied to t=−1t=-1.

Exercises

The base field kk is assumed to be of characteristic zero.

Unless explicitly stated otherwise, Lie algebras are assumed to be finite dimensional.

We denote by s\mathfrak{s} the Lie algebra sl(2,k)\mathfrak{s}\mathfrak{l}(2, k).

See the exercises for § 1.

Transcribed from the printed volume. Not translated.