Bourbaki

§ 5. Solvable Lie algebras

Recall that KK henceforth denotes a field of characteristic 0 and that all Lie algebras are assumed to be finite-dimensional over KK.†

1. Definition of solvable Lie algebras

Definition 1

A Lie algebra gg is called solvable if its kth derived algebra DkgD^k g is zero for sufficiently large kk.

A nilpotent Lie algebra is solvable.

Proposition 1

Subalgebras and quotient algebras of a solvable Lie algebra are solvable. Every extension of a solvable algebra by a solvable algebra is solvable. Every finite product of solvable algebras is solvable.

Let gg be a Lie algebra, g′g' a subalgebra, hh an ideal of gg, t=g/ht = g/h and ϕ\phi the canonical mapping of gg onto tt. If gg is solvable then Dkg={0}D^k g = \{0\} for some integer kk, hence Dkg′⊂Dkg={0}D^k g' \subset D^k g = \{0\}, Dkt=ϕ(Dkg)={0}D^k t = \phi(D^k g) = \{0\} and hence g′g' and tt are solvable. If hh and tt are solvable there exist integers s,ts, t such that

Dsh=Dtt={0}; D^s h = D^t t = \{0\};

then Dtg⊂hD^t g \subset h, hence Ds+tg=Ds(Dtg)⊂Dsh={0}D^{s+t} g = D^s(D^t g) \subset D^s h = \{0\} and gg is solvable. The last assertion follows from the second by induction on the number of factors.

Proposition 2

Let gg be a Lie algebra. The following conditions are equivalent:

(a) gg is solvable; (b) there exists a decreasing sequence g=g0⊃g1⊃⋯⊃gn={0}g = g_0 \supset g_1 \supset \cdots \supset g_n = \{0\} of ideals of gg such that the algebras gi/gi+1g_i/g_{i+1} are commutative (i=0,1,…,n−1i = 0, 1, \ldots, n-1); (c) there exists a decreasing sequence g=g0′⊃g1′⊃⋯⊃gp′={0}g = g'_0 \supset g'_1 \supset \cdots \supset g'_p = \{0\} of subalgebras of gg such that gi+1′g'_{i+1} is an ideal of gi′g'_i and gi′/gi+1′g'_i/g'_{i+1} is commutative (i=0,1,…,p−1i = 0, 1, \ldots, p-1); (d) there exists a decreasing sequence g=g0′′⊃g1′′⊃⋯⊃gq′′={0}g = g''_0 \supset g''_1 \supset \cdots \supset g''_q = \{0\} of subalgebras of gg such that gi+1′′g''_{i+1} is an ideal of gi′′g''_i of codimension 1 (i=0,1,…,q−1i = 0, 1, \ldots, q-1).

(a) ⇒\Rightarrow (b): it suffices to consider the sequence of derived ideals of gg. (b) ⇒\Rightarrow (c): this is obvious. (c) ⇒\Rightarrow (d): suppose that condition (c) holds; every vector subspace of gi′g'_i containing gi+1′g'_{i+1} is an ideal of gi′g'_i, whence immediately (d). (d) ⇒\Rightarrow (a): this follows immediately from the fact that an extension of a solvable algebra by a solvable algebra is solvable.

† The reader will note that the hypothesis on the characteristic of KK is not used in nos. 1 and 2 of this paragraph.

Examples of solvable Lie algebras

I. Let gg be a 2-dimensional vector space over KK and (e1,e2)(e_1, e_2) a basis of gg. There exists one and only one alternating bilinear multiplication (x,y)↦[x,y](x, y) \mapsto [x, y] on gg such that [e1,e2]=e2[e_1, e_2] = e_2. It is easily verified that gg is thus given a solvable Lie algebra structure. Now let hh be a non-commutative Lie algebra of dimension 2 over KK. We show that hh is isomorphic to gg. Let (f1,f2)(f_1, f_2) be a basis of hh. The element [f1,f2][f_1, f_2] is non-zero (otherwise hh would be commutative) and hence it generates a 1-dimensional subspace tt of hh. Then [h,h]=t[h, h] = t. Let (e1′,e2′)(e'_1, e'_2) be a basis of hh such that e2′∈te'_2 \in t. Then [e1′,e2′]=λe2′[e'_1, e'_2] = \lambda e'_2 with λ≠0\lambda \neq 0. Replacing e1′e'_1 by λ−1e1\lambda^{-1} e_1, it can be assumed that λ=1\lambda = 1, whence our assertion.

II. Formulae (5) of § 1 prove that Dt(n,K)=n(n,K)\mathscr{D}t(n, K) = n(n, K). As n(n,K)n(n, K) is nilpotent and hence solvable, t(n,K)t(n, K) is solvable. Therefore st(n,K)st(n, K) is solvable. In particular, st(2,K)st(2, K) is isomorphic to the algebra of Example I.

2. Radical of a Lie algebra

Let a,ba, b be two solvable ideals of a Lie algebra gg. The algebra (a+b)/b(a + b)/b is isomorphic to a/(a∩b)a/(a \cap b) and hence is solvable and a+ba + b, which is an extension of (a+b)/b(a + b)/b by bb, is also solvable (Proposition 1). It follows that a maximal solvable ideal of gg contains every solvable ideal of gg and hence gg has a largest solvable ideal. This enables us to make the following definition:

Definition 2

The radical of a Lie algebra is its largest solvable ideal.

Proposition 3

The radical rr of a Lie algebra gg is the smallest ideal of gg such that g/rg/r has radical {0}\{0\}.

Let aa be an ideal of gg and ϕ\phi the canonical mapping of gg onto g/ag/a. If the radical of g/ag/a is zero, then ϕ(r)\phi(r), which is a solvable ideal of g/ag/a, is zero; hence r⊂ar \subset a.

On the other hand, the inverse image ϕ−1(r′)\phi^{-1}(r') of the radical r′r' of g/rg/r is an ideal of gg which is solvable by Proposition 1 and hence is equal to rr; therefore r′={0}r' = \{0\}.

Proposition 4

Let g1,…,gng_1, \ldots, g_n be Lie algebras. The radical rr of the product of the gig_i is the product of the radicals rir_i of the gig_i.

The product r′r' of the rir_i is a solvable ideal (Proposition 1) and hence r′⊂rr' \subset r. The canonical image of rr in gig_i is a solvable ideal of gig_i and hence is contained in rir_i; hence r⊂r′r \subset r'.

3. Nilpotent radical of a Lie algebra

Definition 3

Let gg be a Lie algebra. The nilpotent radical of gg is the intersection of the kernels of the finite-dimensional simple representations of gg.

Remark

(1) Let ss be the nilpotent radical of gg. As every decreasing sequence of vector subspaces of gg is stationary, there exists a finite number of finite-dimensional simple representations of gg whose kernels have intersection ss.

The direct sum of these representations is semi-simple and has kernel s. It follows that the set of kernels of finite-dimensional semi-simple representations of g has a least element, namely s.

(2) By Proposition 4 (c) of § 4, no. 3, s is also the intersection of the largest nilpotency ideals of the finite-dimensional representations of g. In particular, s is contained in the largest nilpotent ideal of g and is therefore a nilpotent ideal of g.

(3) Every linear form λ\lambda on g which is zero on Dg\mathscr{D}g is a simple representation (with space K) of g, whence λ(s)={0}\lambda(s) = \{0\}. It follows that s⊂Dgs \subset \mathscr{D}g. On the other hand, s is contained in the radical r of g by Remark 2. We shall prove that s=r∩Dgs = r \cap \mathscr{D}g.

Lemma 1

Let V be a finite-dimensional vector space over K, g a subalgebra of gl(V) such that V is a simple g-module and a a commutative ideal of g. Then a∩Dg={0}a \cap \mathscr{D}g = \{0\}. Let S be the subalgebra of L(V)\mathscr{L}(V) generated by 1 and a.

If b is an ideal of g contained in a such that Tr⁡bs=0\operatorname{Tr} bs = 0 for all b∈bb \in b and all s∈Ss \in S, then in particular, by definition of S, Tr⁡(bn)=0\operatorname{Tr}(b^n) = 0 for every integer n>0n > 0 and hence b is nilpotent (Algebra, Chapter VII, § 5, no. 5, Corollary 4 to Proposition 13); as the elements of b are all nilpotent, b={0}b = \{0\} (§ 4, no. 3, Lemma 2). We first apply this to the ideal [g,a][g, a] of g. If x∈g,a∈a,s∈Sx \in g, a \in a, s \in S, then Tr⁡[x,a]s=Tr⁡(xas−axs)=Tr⁡x(as−sa)=0\operatorname{Tr}[x, a]s = \operatorname{Tr}(xas - axs) = \operatorname{Tr} x(as - sa) = 0 since as=saas = sa; hence [g,a]={0}[g, a] = \{0\}. Hence the elements of g commute with those of a and hence also with those of S. If x,yx, y belong to g and s∈Ss \in S, then

Tr⁡[x,y]s=Tr⁡(xys−yxs)=Tr⁡x(ys−sy)=0 \operatorname{Tr}[x, y]s = \operatorname{Tr}(xys - yxs) = \operatorname{Tr} x(ys - sy) = 0

since ys=syys = sy; then taking b to be the ideal Dg∩a\mathscr{D}g \cap a, it follows that Dg∩a={0}\mathscr{D}g \cap a = \{0\}.

Theorem 1

Let g be a Lie algebra, r its radical and s its nilpotent radical. Then s=Dg∩rs = \mathscr{D}g \cap r.

We already know that s⊂Dg∩rs \subset \mathscr{D}g \cap r. Hence it will suffice to show that if ρ\rho is a finite-dimensional simple representation of g then ρ(Dg∩r)={0}\rho(\mathscr{D}g \cap r) = \{0\}. Let k be the least integer ≥0\geq 0 such that ρ(Dk+1r)={0}\rho(\mathscr{D}^{k+1}r) = \{0\}; we write g′=ρ(g)g' = \rho(g), a′=ρ(Dkr)a' = \rho(D^k r); as Dkr\mathscr{D}^k r is an ideal of g, a′a' is an ideal of g′g'; this ideal is commutative since ρ(Dk+1r)={0}\rho(\mathscr{D}^{k+1}r) = \{0\}. If V is the space of ρ\rho, g′⊂gl⁡(V)g' \subset \operatorname{gl}(V) and V is a simple g′g'-module. Then ρ(Dg∩Dkr)⊂Dg′∩a′={0}\rho(\mathscr{D}g \cap \mathscr{D}^k r) \subset \mathscr{D}g' \cap a' = \{0\}. If k>0k > 0, then Dkr⊂Dg\mathscr{D}^k r \subset \mathscr{D}g and ρ(Dkr)={0}\rho(\mathscr{D}^k r) = \{0\}, contrary to the definition of k. Hence k=0k = 0, that is

ρ(Dg∩r)={0}. \rho(\mathscr{D}g \cap r) = \{0\}.

Corollary 1

Let g be a solvable Lie algebra. The nilpotent radical of g is Dg\mathscr{D}g. If ρ\rho is a finite-dimensional simple representation of g, ρ(g)\rho(g) is commutative and the associative algebra L generated by 1 and ρ(g)\rho(g) is a field of finite degree over K.

Here r=gr = g, whence s=Dgs = \mathscr{D}g. Hence φ(Dg)={0}\varphi(\mathscr{D}g) = \{0\}, which shows that g′=ρ(g)g' = \rho(g) is commutative. Every element ≠0\neq 0 of LL is invertible by Schur’s Lemma; hence LL is a field.

Corollary 2 (Lie’s Theorem). Let gg be a solvable Lie algebra; suppose that KK is algebraically closed. Let MM be a gg-module of finite dimension over KK and let (Mi)0≤i≤r(M_i)_{0 \leq i \leq r} be a Jordan-Hölder series of MM. Then Mi−1/MiM_{i-1}/M_i is of dimension 1 over KK for 1≤i≤r1 \leq i \leq r and, for all x∈gx \in g, xMi−1/Mi=λi(x)⋅1x_{M_{i-1}/M_i} = \lambda_i(x) \cdot 1, where λi\lambda_i is a linear form on gg which is zero on Dg\mathscr{D}g. In particular, every simple gg-module of finite dimension over KK is in fact of dimension 1.

Let ρi\rho_i be the representation of gg on Mi−1/MiM_{i-1}/M_i. The associative algebra LiL_i generated by 1 and ρi(g)\rho_i(g) is a field, a finite extension of KK and therefore equal to KK; and Mi−1/MiM_{i-1}/M_i is a simple LiL_i-module, whence dim⁡Mi−1/Mi=1\dim M_{i-1}/M_i = 1. The rest of the corollary is obvious.

Remark

(1) If (Mi)0≤i≤r(M_i)_{0 \leq i \leq r} is replaced by another Jordan-Hölder series of MM, the sequence (λ1,…,λr)(\lambda_1, \ldots, \lambda_r) is replaced by a sequence of the form (λπ(1),…,λπ(r))(\lambda_{\pi(1)}, \ldots, \lambda_{\pi(r)}), where π\pi is a permutation of {1,…,r}\{1, \ldots, r\}, as follows from the Jordan-Hölder Theorem.

(2) Let (e1,…,er)(e_1, \ldots, e_r) be a basis of MM such that ei∈Mi−1,ei∉Mie_i \in M_{i-1}, e_i \notin M_i (1≤i≤r1 \leq i \leq r). If x∈gx \in g the endomorphism of MM corresponding to xx is represented with respect to this basis by a triangular matrix whose diagonal coefficients are

λ1(x),…,λr(x). \lambda_1(x), \ldots, \lambda_r(x).

Corollary 3

Suppose that KK is algebraically closed. If gg is an rr-dimensional solvable Lie algebra, every ideal of gg is a term of a decreasing sequence of ideals of dimensions r,r−1,…,0r, r-1, \ldots, 0.

Every ideal is part of a Jordan-Hölder series of gg, considered as the space of the adjoint representation (Algebra, Chapter I, § 6, no. 14, Corollary to Theorem 8); then it suffices to apply Corollary 2.

Corollary 4

Suppose that K=RK = \mathbf{R}. Let gg be a solvable Lie algebra. Every simple representation of gg is of dimension ≤2\leq 2. Every ideal of gg is a term of a decreasing sequence (gi)0≤i≤m(g_i)_{0 \leq i \leq m} of ideals such that g0=g,gm={0},dim⁡gi−1/gi≤2g_0 = g, g_m = \{0\}, \dim g_{i-1}/g_i \leq 2 (1≤i≤m1 \leq i \leq m).

This is proved in a similar way to that for Corollaries 2 and 3, using the fact that every algebraic extension of R\mathbf{R} is of degree ≤2\leq 2.

Corollary 5

For a Lie algebra gg to be solvable, it is necessary and sufficient that Dg\mathscr{D}g be nilpotent.

The condition is necessary by Corollary 1. It is sufficient since g/Dgg/\mathscr{D}g is commutative.

Corollary 6

Let φ\varphi be a finite-dimensional representation of a Lie algebra gg. Let* r be the radical of g. Every element x∈rx \in r such that ρ(x)\rho(x) is nilpotent belongs to the largest nilpotency ideal nn of ρ\rho.

Let V be the space of ρ\rho; let (Vi)0≤i≤r(V_i)_{0 \leq i \leq r} be a Jordan-Hölder series for the r-module structure on V and let ρi\rho_i be the representation of r with space Vi/Vi−1V_i / V_{i-1} (1≤i≤r1 \leq i \leq r). If ρ(x)\rho(x) is nilpotent, so is ρi(x)\rho_i(x); as for all ii the algebra generated by ρi(x)\rho_i(x) is a field, ρi(x)=0\rho_i(x) = 0. Conversely, if ρi(x)=0\rho_i(x) = 0 for all ii, ρ(x)=0\rho(x) = 0. This shows that the set aa of x∈rx \in r such that ρ(x)\rho(x) is nilpotent is an ideal of r. On the other hand, [g,a]⊂Dg∩r⊂n∩r⊂a[g, a] \subset \mathscr{D}g \cap r \subset n \cap r \subset a and hence aa is an ideal of g. This proves that a⊂na \subset n.

Corollary 7

Let g be a Lie algebra and r its radical. The following four sets are identical: (a) the largest nilpotent ideal of g; (b) the largest nilpotent ideal of r; (c) the set of x∈rx \in r such that adgx\mathrm{ad}_g x is nilpotent; (d) the set of x∈rx \in r such that adrx\mathrm{ad}_r x is nilpotent.

Let these sets be denoted by a,b,c,da, b, c, d. The inclusions a⊂b⊂d⊂ca \subset b \subset d \subset c are clear. c⊂ac \subset a by Corollary 6 applied to the adjoint representation of g.

4. A criterion for solvability

Lemma 2

Let xx be an endomorphism of a finite-dimensional vector space V and s (resp. n) its semi-simple (resp. nilpotent) component (cf. Algebra, Chapter VIII, § 9, no. 4, Definition 4). Let ad x,ad s,ad n\mathrm{ad}\, x, \mathrm{ad}\, s, \mathrm{ad}\, n be the respective images of x,s,nx, s, n in the adjoint representation of gl(V)\mathfrak{gl}(V). Then ad s\mathrm{ad}\, s (resp. ad n\mathrm{ad}\, n) is the semi-simple (resp. nilpotent) component of ad x\mathrm{ad}\, x and is equal to a polynomial in ad x\mathrm{ad}\, x with coefficients in K and no constant term.

We know that ad x=ad s+ad n,[ad s,ad n]=0\mathrm{ad}\, x = \mathrm{ad}\, s + \mathrm{ad}\, n, [\mathrm{ad}\, s, \mathrm{ad}\, n] = 0 and ad n\mathrm{ad}\, n is nilpotent (§4§ 4, Lemma 1). We show that ad s\mathrm{ad}\, s is semi-simple. It suffices to do this when K is algebraically closed (cf. Algebra, Chapter VIII, § 9, no. 2, Proposition 3). Then let (ei)1≤i≤n(e_i)_{1 \leq i \leq n} be a basis of V such that s(ei)=λieis(e_i) = \lambda_i e_i (λi∈K\lambda_i \in K). Let (Eij)(E_{ij}) be the canonical basis of Mn(K)=gl(V)M_n(K) = \mathfrak{gl}(V). By formulae (5) of §1§ 1,

(ad s)⋅Eij=(λi−λj)Eij (\mathrm{ad}\, s)\cdot E_{ij} = (\lambda_i - \lambda_j)E_{ij}

and hence ad s\mathrm{ad}\, s is semi-simple. The last assertion of the lemma follows from Algebra, Chapter VIII, § 9, no. 4, Proposition 8.

Lemma 3

Let M be a finite-dimensional vector space, A and B two vector subspaces of gl(M)\mathfrak{gl}(M) such that B⊂AB \subset A and T the set of t∈gl(M)t \in \mathfrak{gl}(M) such that [t,A]⊂B[t, A] \subset B. If z∈Tz \in T is such that Tr(zu)=0\mathrm{Tr}(zu) = 0 for all u∈Tu \in T, then zz is nilpotent.

It suffices to prove this when K is algebraically closed, which we shall assume henceforth. Let s and n be the semi-simple and nilpotent components of z and let (ei)(e_i) be a basis of M such that s(ei)=λieis(e_i) = \lambda_i e_i (λi∈K\lambda_i \in K). Let V⊂KV \subset K be the vector space over Q\mathbf{Q} generated by the λi\lambda_i. We need to prove that V={0}V = \{0\}. Let f be a Q\mathbf{Q}-linear form on V and let t be the endomorphism of M such that

tei=f(λi)eite_i = f(\lambda_i)e_i. If (Eij)(E_{ij}) is the canonical basis of gl(M)\mathfrak{gl}(M) defined by Eijek=δjkeiE_{ij}e_k = \delta_{jk}e_i, then

(ad s)Eij=(λi−λj)Eij(ad t)Eij=(f(λi)−f(λj))Eij. \begin{align*} (\mathrm{ad}\ s)E_{ij} &= (\lambda_i - \lambda_j)E_{ij} \\ (\mathrm{ad}\ t)E_{ij} &= (f(\lambda_i) - f(\lambda_j))E_{ij}. \end{align*}

There exists a polynomial P with no constant term and with coefficients in K such that P(λi−λj)=f(λi)−f(λj)P(\lambda_i - \lambda_j) = f(\lambda_i) - f(\lambda_j) for all i and j (for if λi−λj=λh−λk\lambda_i - \lambda_j = \lambda_h - \lambda_k, then f(λi)−f(λj)=f(λh)−f(λk)f(\lambda_i) - f(\lambda_j) = f(\lambda_h) - f(\lambda_k) and, if λi−λj=0\lambda_i - \lambda_j = 0, f(λi)−f(λj)=0f(\lambda_i) - f(\lambda_j) = 0). Then ad t=P(ad s)\mathrm{ad}\ t = P(\mathrm{ad}\ s). On the other hand, ad s\mathrm{ad}\ s is a polynomial with no constant term in ad z\mathrm{ad}\ z. Now (ad z)(A)⊂B(\mathrm{ad}\ z)(A) \subset B, whence also (ad t)(A)⊂B(\mathrm{ad}\ t)(A) \subset B. By the hypothesis 0=Tr(zt)=∑λif(λi)0 = \mathrm{Tr}(zt) = \sum \lambda_i f(\lambda_i), whence 0=f(Tr(zt))=∑f(λi)20 = f(\mathrm{Tr}(zt)) = \sum f(\lambda_i)^2. Since the f(λi)f(\lambda_i) are rational numbers, f=0f = 0, which completes the proof.

Theorem 2 (Cartan's criterion)

Let g be a Lie algebra, M a finite-dimensional vector space, ρ a representation of g on M and β the bilinear form on g associated with ρ. Then ρ(g) is solvable if and only if D\mathscr{D}g is orthogonal to g with respect to β.

It can obviously be reduced to the case where g is a Lie subalgebra of gl(M)\mathfrak{gl}(M) and ρ is the identity mapping. If g is solvable, D\mathscr{D}g is contained in the largest nilpotency ideal of the identity representation of g (Theorem 1) and hence is orthogonal to g with respect to β (§ 4, Proposition 4 (d)). Suppose that D\mathscr{D}g is orthogonal to g with respect to β. We prove that g is solvable. Let T be the set of t∈gl(M)t \in \mathfrak{gl}(M) such that [t,g]⊂Dg[t, g] \subset \mathscr{D}g. If t∈Tt \in T and x, y belong to g, then [t,x]∈Dg[t, x] \in \mathscr{D}g and hence

Tr(t[x,y])=β([t,x],y)=0 \mathrm{Tr}(t[x, y]) = \beta([t, x], y) = 0
whence by linearity Tr(tu)=0\mathrm{Tr}(tu) = 0 for all u∈Dgu \in \mathscr{D}g. Also, clearly Dg⊂T\mathscr{D}g \subset T. Hence (Lemma 3) every element of D\mathscr{D}g is nilpotent. It follows that D\mathscr{D}g is nilpotent (§ 4, Corollary 3 to Theorem 1) and hence that g is solvable (no. 3, Corollary 5 to Theorem 1).

5. Further properties of the radical

Proposition 5

Let g be a Lie algebra and r its radical.* (a) If ρ is a finite-dimensional representation of g and β is the associated bilinear form, r and D\mathscr{D}g are orthogonal with respect to β. (b) r is the orthogonal of D\mathscr{D}g with respect to the Killing form. Let x, y be in g, z∈rz \in r. Then [y,z]∈Dg∩r[y, z] \in \mathscr{D}g \cap r and hence

β([x,y],z)=β(x,[y,z])=0 \beta([x, y], z) = \beta(x, [y, z]) = 0
(Theorem 1). Hence (a). Let r' be the orthogonal of D\mathscr{D}g with respect to the Killing form. It is an ideal of g (§ 3, no. 6, Proposition 7 (a)) which contains r by the above. On the other hand, the image s of r' under the adjoint representation of g is solvable (Theorem 2) and hence r' is solvable being a central extension of s. Hence r' ⊂ r.

Corollary 1

Let g be a Lie algebra. Then g is solvable if and only if Dg\mathscr{D}g is orthogonal to g with respect to the Killing form.

This is an immediate consequence of Proposition 5 (b).

Corollary 2

The radical r of a Lie algebra g is a characteristic ideal.

Dg\mathscr{D}g is a characteristic ideal and the Killing form is completely invariant (§ 3, no. 6, Proposition 10). Hence the orthogonal of Dg\mathscr{D}g with respect to the Killing form is a characteristic ideal (§ 3, no. 6, Proposition 7 (b)).

Corollary 3

Let g be a Lie algebra, r its radical and a an ideal of g. Then the radical of a is equal to r∩ar \cap a.

r ∩ a is a solvable ideal of a and hence is contained in the radical r' of a. Conversely, r' is an ideal of g (Corollary 2 and § 1, no. 4, Proposition 2) and hence r' ⊂ r.

Corollary 2 can be made more precise as follows:

Proposition 6

Let g be a Lie algebra, r its radical and n its largest nilpotent ideal. Every derivation of g maps r into n.

Let D be a derivation of g. Let g' = g + Kx_0 be a Lie algebra in which g is an ideal of codimension 1 such that Dx = [x_0, x] for all x ∈ g (§ 1, no. 8, Example 1). By Corollary 3 to Proposition 5, r is contained in the radical r' of g'. Then D(r) = [x_0, r] ⊂ [g', g'] ∩ r' = s'. For all x ∈ s', ad_{g'} x is nilpotent (Theorem 1). Hence, for all x ∈ s' ∩ g, ad_g x is nilpotent. Hence D(r) is contained in the nilpotent ideal s' ∩ g of g.

Corollary

The largest nilpotent ideal of a Lie algebra is a characteristic ideal.

Remark

To summarize some of the above results, note that, if r, n, s, t denote respectively the radical of g, the largest nilpotent ideal of g, the nilpotent radical of g and the orthogonal of g with respect to the Killing form, then

r⊃t⊃n⊃s. r \supset t \supset n \supset s.

The inclusion r ⊃ t follows from Proposition 5 (b). The inclusion t ⊃ n follows from § 4, no. 4, Proposition 6 (b). The inclusion n ⊃ s has been pointed out in Remark 2 of no. 3.

6. Extension of the base field

Let g be a Lie K-algebra and K_1 an extension of K. Clearly g_{(K_1)} is solvable if and only if g is solvable, since Dn(g(K1))=(Dng)(K1)\mathscr{D}^n(g_{(K_1)}) = (\mathscr{D}^n g)_{(K_1)}.

Let r be the radical of g. Then r(K1)r_{(K_1)} is the radical of g(K1)g_{(K_1)}. For let β\beta be the Killing form of g. As r is the orthogonal of Dg\mathscr{D}g with respect to β\beta (Proposition 5 (b)), r(K1)r_{(K_1)} is the orthogonal of (Dg)(K1)=D(g(K1))(\mathscr{D}g)_{(K_1)} = \mathscr{D}(g_{(K_1)}) with respect to the form derived from β\beta by extension from K to K1K_1, that is the Killing form of g(K1)g_{(K_1)} (§ 3, no. 8). Our assertion then follows from a further application of Proposition 5 (b).

Exercises

The conventions of § 5 remain valid unless otherwise mentioned.

See the exercises for § 5.

Transcribed from the printed volume. Not translated.