Bourbaki

§ 1. Definition of Lie algebras

1. Algebras

Let M be a unitary module over K with a bilinear mapping (x,y)↦xy(x, y) \mapsto xy of M×MM \times M into M. All the axioms for algebras are satisfied except associativity of multiplication. By an abuse of language, M is called a not necessarily associative algebra over K, or sometimes, when no confusion can arise, an algebra over K. In this no. we shall use the latter notation.

If the K-module M is given the multiplication (x,y)↦yx(x, y) \mapsto yx an algebra is obtained called the opposite of the above algebra.

A sub-K-module N of M which is stable under multiplication is given the structure of an algebra over K in an obvious way. N is called a subalgebra of M. N is called a left (resp. right) ideal of M if the conditions x∈N,y∈Mx \in N, y \in M imply yx∈Nyx \in N (resp. xy∈Nxy \in N). If N is both a left ideal and a right ideal of M, N is called a two-sided ideal of M. In this case the multiplication on M enables us to define, on passing to the quotient, a bilinear multiplication on the quotient module M/NM/N such that M/NM/N has an algebra structure. M/NM/N is called the quotient algebra of M by N.

† The propositions proved in this chapter depend only on the properties established in Books I to VI and on certain results of Commutative Algebra, Chapter III, § 2.

Let M1M_1 and M2M_2 be two algebras over KK and ϕ\phi a mapping of M1M_1 into M2M_2. ϕ\phi is called a homomorphism if ϕ\phi is KK-linear and ϕ(xy)=ϕ(x)ϕ(y)\phi(xy) = \phi(x)\phi(y) for x∈M1,y∈M1x \in M_1, y \in M_1. The kernel NN of ϕ\phi is a two-sided ideal of M1M_1 and the image of ϕ\phi is a subalgebra of M2M_2. On passing to the quotient, ϕ\phi defines an isomorphism of the algebra M1/NM_1/N onto the algebra ϕ(M1)\phi(M_1).

Let MM be an algebra over KK. A mapping DD of MM into MM is called a derivation of MM if it is KK-linear and D(xy)=(Dx)y+x(Dy)D(xy) = (Dx)y + x(Dy) for all x∈Mx \in M and y∈My \in M. This definition generalizes Definition 3 of Algebra, Chapter IV, § 4, no. 3. The kernel of a derivation of MM is a subalgebra of MM. If D1D_1 and D2D_2 are derivations of MM, then D1D2−D2D1D_1D_2 - D_2D_1 is a derivation of MM (cf. Algebra, Chapter IV, § 4, no. 3, Proposition 5: the proof of this proposition does not use the associativity of the algebra).

Let M1M_1 and M2M_2 be two algebras over KK. On the product KK-module M=M1×M2M = M_1 \times M_2 we define a multiplication by writing

(x1,x2)(y1,y2)=(x1y1,x2y2), (x_1, x_2)(y_1, y_2) = (x_1y_1, x_2y_2),

for all x1,y1x_1, y_1 in M1M_1, x2,y2x_2, y_2 in M2M_2. The algebra thus defined is called the product algebra of M1M_1 and M2M_2. The mapping x1↦(x1,0)x_1 \mapsto (x_1, 0) (resp. x2↦(0,x2)x_2 \mapsto (0, x_2)) is an isomorphism of M1M_1 (resp. M2M_2) onto a two-sided ideal of MM. Under these isomorphisms M1M_1 and M2M_2 are identified with two-sided ideals of MM. The KK-module MM is then the direct sum of M1M_1 and M2M_2. Conversely, let MM be an algebra over KK and M1,M2M_1, M_2 two two-sided ideals of MM such that MM is the direct sum of M1M_1 and M2M_2. Then M1M2⊂M1∩M2={0}M_1M_2 \subset M_1 \cap M_2 = \{0\}; then, if x1,y1x_1, y_1 belong to M1M_1 and x2,y2x_2, y_2 to M2M_2, then (x1+x2)(y1+y2)=x1y1+x2y2(x_1 + x_2)(y_1 + y_2) = x_1y_1 + x_2y_2, so that MM is identified with the product algebra M1×M2M_1 \times M_2. Every left (resp. right, two-sided) ideal of M1M_1 is a left (resp. right, two-sided) ideal of MM. We leave to the reader the task of formulating the analogous results in the case of an arbitrary finite family of algebras.

Let MM be an algebra over KK and suppose that the KK-module MM admits a basis (aλ)λ∈L(a_\lambda)_{\lambda \in L}. There exists a unique system (γλμν)(λ,μ,ν)∈L×L×L(\gamma_{\lambda \mu \nu})_{(\lambda, \mu, \nu) \in L \times L \times L} of elements of KK such that aλaμ=∑vγλμvava_\lambda a_\mu = \sum_v \gamma_{\lambda \mu v} a_v for all λ,μ\lambda, \mu in LL. The γλμν\gamma_{\lambda \mu \nu} are called the constants of structure of MM with respect to the basis (aλ)(a_\lambda).

Let MM be an algebra over KK, K0K_0 a commutative ring with unit element and ρ\rho a homomorphism of K0K_0 into KK mapping unit element to unit element. Then MM can be considered as an algebra over K0K_0 by writing α.x=ρ(α).x\alpha.x = \rho(\alpha).x for α∈K0,x∈M\alpha \in K_0, x \in M. This is the case in particular when K0K_0 is a subring of KK containing the unit element and ρ\rho is taken to be the inclusion mapping of K0K_0 into KK.

Let MM be an algebra over KK, K1K_1 a commutative ring with unit element and σ\sigma a homomorphism of KK into K1K_1 mapping unit element to unit element. Let M(K1,σ)=M(K1)M_{(K_1, \sigma)} = M_{(K_1)} be the K1K_1-module derived from MM by extending the ring of scalars to K1K_1 (Algebra, Chapter II, § 5). The product on MM defines canonically a K1K_1-bilinear mapping of M(K1)×M(K1)M_{(K_1)} \times M_{(K_1)} into M(K1)M_{(K_1)} (Algebra, Chapter IX, § 1, no. 4) such that M(K1)M_{(K_1)} is given the structure of an algebra over K1K_1 (which is said to be derived from MM by extending the ring of scalars to K1K_1). This is the case in particular when KK is a subring of K1K_1 containing the unit element and σ\sigma the inclusion mapping of KK into K1K_1.

2. Lie algebras

Definition 1

An algebra g over K is called a Lie algebra over K if its multiplication (denoted by (x,y)↦[x,y](x, y) \mapsto [x, y]) satisfies the identities:

(1)

[x,x]=0 [x, x] = 0

(2)

[x,[y,z]]+[y,[z,x]]+[z,[x,y]]=0 [x, [y, z]] + [y, [z, x]] + [z, [x, y]] = 0

for all x,y,zx, y, z in g.

The product [x,y][x, y] is called the bracket of xx and yy. Identity (2) is called the Jacobi identity.

The bracket [x,y][x, y] is an alternating bilinear function of xx and yy. We have the identity:

(3)

[x,y]=−[y,x] [x, y] = -[y, x]

so that the Jacobi identity can be written:

(4)

[x,[y,z]]=[[x,y],z]+[y,[x,z]]. [x, [y, z]] = [[x, y], z] + [y, [x, z]].

Every subalgebra and every quotient algebra of a Lie algebra is a Lie algebra. Every product of Lie algebras is a Lie algebra. If gg is a Lie algebra, the opposite algebra g0g^0 is a Lie algebra and the mapping x↦−xx \mapsto -x an isomorphism of gg onto g0g^0, by virtue of identity (3).

Example 1

Let LL be an associative algebra over KK. The bracket [x,y]=xy−yx[x, y] = xy - yx is a bilinear function of xx and yy. It is easily verified that the law of composition (x,y)↦[x,y](x, y) \mapsto [x, y] on the KK-module LL makes LL into a Lie algebra over KK.

Example 2

In Example 1 choose LL to be the associative algebra of endomorphisms of a KK-module EE. We obtain the Lie algebra of endomorphisms of EE, denoted by gl(E)gl(E). (If E=KnE = K^n, the Lie algebra gl(E)gl(E) is denoted by gl(n,K)gl(n, K).)

Every Lie subalgebra of gl(E)gl(E) is a Lie algebra over KK. In particular: (1) If EE is given a (not necessarily associative) algebra structure, the derivations of EE form a Lie algebra over KK. (2) If EE admits a finite basis, the endomorphisms of EE of zero trace form a Lie algebra over KK denoted by sl(E)sl(E) (or sl(n,K)sl(n, K) if E=KnE = K^n).

Example 3

The set Mn(K)M_n(K) of square matrices of order nn can be considered as a Lie algebra over K canonically isomorphic to gl(n, K). Let (Eij)(E_{ij}) be the canonical basis of Mn(K)\mathbf{M}_n(K) (Algebra, Chapter II, § 10, no. 3). It follows easily that:

{[Eij,Ekl]=0if j≠k and i≠l[Eij,Ejl]=Eilif i≠l[Eij,Ekt]=−Ekjif j≠k[Eij,Eji]=Eii−Ejj \begin{cases} [E_{ij}, E_{kl}] = 0 & \text{if } j \neq k \text{ and } i \neq l \\ [E_{ij}, E_{jl}] = E_{il} & \text{if } i \neq l \\ [E_{ij}, E_{kt}] = -E_{kj} & \text{if } j \neq k \\ [E_{ij}, E_{ji}] = E_{ii} - E_{jj} \end{cases}

(5)

The Lie subalgebra of Mn(K)\mathbf{M}_n(K) consisting of the triangular matrices (resp. triangular matrices of zero trace, resp. triangular matrices of zero diagonal) is denoted by t(n,K)t(n, K) (resp. st(n, K), resp. n(n, K)) (Algebra, Chapter II, § 10; no. 7).

Example 3. Let V be an infinitely differentiable real manifold. The differential operators with infinitely differentiable real coefficients constitute an associative algebra over R\mathbf{R} and hence, by Example 1, a Lie algebra Δ\Delta over R\mathbf{R}. The bracket of two infinitely differentiable vector fields on V is an infinitely differentiable vector field and hence the infinitely differentiable vector fields on V constitute a Lie subalgebra f\mathfrak{f} of Δ\Delta. If V is a real Lie group, the left invariant vector fields constitute a Lie subalgebra gg of f\mathfrak{f} called the Lie algebra of V. The vector space gg is identified with the tangent space to V at ee (the identity element of V). Let V' be another real Lie group, e′e' its identity element and g′g' its Lie algebra. Every analytic homomorphism of V into V' defines a linear mapping of the tangent space to V at ee into the tangent space to V' at e′e'; this mapping is a homomorphism of the Lie algebra gg into the Lie algebra g′g'. If V is the linear group of a finite-dimensional real vector space E there exists a canonical isomorphism of gl(E)gl(E) onto the Lie algebra gg of V, under which gg is identified with gl(E)gl(E).

Definition 2

Let g be a Lie algebra and x an element of g. The linear mapping y↦[x,y]y \mapsto [x, y] of g into g is called the adjoint linear mapping of x and is denoted by ad⁡gx\operatorname{ad}_g x or ad⁡x\operatorname{ad} x.

Proposition 1

Let g be a Lie algebra. For all x∈gx \in g, ad⁡x\operatorname{ad} x is a derivation. The mapping x↦ad⁡xx \mapsto \operatorname{ad} x is a homomorphism of the Lie algebra g into the Lie algebra d\mathfrak{d} of derivations of g. If D∈dD \in \mathfrak{d} and x∈gx \in g, [D,ad⁡x]=ad⁡(Dx)[D, \operatorname{ad} x] = \operatorname{ad}(Dx).

Identity (4) can be written:

(ad⁡x)⋅[y,z]=[(ad⁡x)⋅y,z]+[y,(ad⁡x)⋅z] (\operatorname{ad} x) \cdot [y, z] = [(\operatorname{ad} x) \cdot y, z] + [y, (\operatorname{ad} x) \cdot z]

or:

(ad⁡[x,y])⋅z=(ad⁡x)⋅((ad⁡y)⋅z)−(ad⁡y)⋅((ad⁡x)⋅z) (\operatorname{ad}[x, y]) \cdot z = (\operatorname{ad} x) \cdot ((\operatorname{ad} y) \cdot z) - (\operatorname{ad} y) \cdot ((\operatorname{ad} x) \cdot z)

whence the first two assertions. On the other hand, if D∈dD \in \mathfrak{d}, x∈gx \in g, y∈gy \in g, then [D,ad⁡x]⋅y=D([x,y])−[x,Dy]=[Dx,y]=(ad⁡Dx)⋅y[D, \operatorname{ad} x] \cdot y = D([x, y]) - [x, Dy] = [Dx, y] = (\operatorname{ad} Dx) \cdot y, whence the last assertion.

The mapping ad⁡x\operatorname{ad} x is also called the inner derivation defined by xx.

3. Commutative Lie algebras

Definition 3

Two elements x, y of a Lie algebra are said to be permutable if [x, y] = 0. g is said to be commutative if any two of its elements are permutable.

Example 1

Let L be an associative algebra and g the Lie algebra defined by it (no. 2, Example 1). Two elements x, y are permutable in g if and only if xy = yx in L.

Example 2. If a real Lie group G is commutative, its Lie algebra is commutative.

Every K-module can obviously be given a unique commutative Lie algebra structure over K.

If g is a Lie algebra, every monogenous submodule of g is a commutative Lie subalgebra of g.

4. Ideals

It follows from identity (3) that in a Lie algebra g there is no distinction between left ideals and right ideals, every ideal being two-sided. We therefore speak simply of ideals.

Example. Let G be a Lie group, g its Lie algebra and H a Lie subgroup of G. Every left invariant vector field on H defines canonically a left invariant vector field on G, whence there is a canonical injection of the Lie algebra h of H into g; h is identified with a Lie subalgebra of g under this injection. If H is normal in G, the canonical image of h in g is an ideal of g.

An ideal of g is a submodule of g which is stable under the inner derivations of g.

Definition 4

A submodule of g which is stable under every derivation of g is called a characteristic ideal of g.

Proposition 2

Let g be a Lie algebra, a an ideal (resp. a characteristic ideal) of g and b a characteristic ideal of a. Then b is an ideal (resp. a characteristic ideal) of g.

Every inner derivation (resp. every derivation) of g leaves a stable and induces on a a derivation and hence leaves b stable.

Let g be a Lie algebra. If a and b are ideals of g, a + b and a ∩ b are ideals of g.

Let a and b be two submodules of g. By an abuse of notation, the submodule of g generated by the elements of the form [x, y] (x ∈ a, y ∈ b) is denoted by [a, b]. We have [a, b] = [b, a] by identity (3). If z ∈ g, [z, a], or [a, z], denotes the submodule [Kz, a] = (ad z)(a).

Proposition 3

If a and b are ideals (resp. characteristic ideals) of g, [a, b] is an ideal (resp. a characteristic ideal) of g.

Let D be an inner derivation (resp. a derivation) of g. If x∈ax \in a and y∈by \in b, then

D([x,y])=[Dx,y]+[x,Dy]∈[a,b]. D([x, y]) = [Dx, y] + [x, Dy] \in [a, b].
Hence the proposition.

If a is a submodule of g, the set of x∈gx \in g such that (ad x).a⊂a(\mathrm{ad}\ x).a \subset a is a subalgebra n of g called the normalizer of a in g. If further a is a subalgebra of g, then a⊂na \subset n and a is an ideal of n.

5. Derived series, lower central series

The characteristic ideal [g,g][g, g] is called the derived ideal of a Lie algebra g and denoted by Dg\mathscr{D}g.

Every submodule of g containing Dg\mathscr{D}g is an ideal of g.

The derived series of g is the decreasing sequence D0g,D1g,…\mathscr{D}^0g, \mathscr{D}^1g, \ldots of characteristic ideals of g defined inductively as follows: (1) D0g=g\mathscr{D}^0g = g; (2) Dp+1g=[Dpg,Dpg]\mathscr{D}^{p+1}g = [\mathscr{D}^pg, \mathscr{D}^pg].

The lower central series of g is the decreasing sequence C1g,C2g,…\mathscr{C}^1g, \mathscr{C}^2g, \ldots of characteristic ideals of g defined inductively as follows: (1) C1g=g\mathscr{C}^1g = g; (2) Cp+1g=[g,Cpg]\mathscr{C}^{p+1}g = [g, \mathscr{C}^pg]. Then C2g=Dg\mathscr{C}^2g = \mathscr{D}g and Cp+1g⊃Dpg\mathscr{C}^{p+1}g \supset \mathscr{D}^pg for all pp, as is immediately seen by induction on pp.

Proposition 4

Let g and h be two Lie algebras over K and f a homomorphism of g onto h. Then f(Dpg)=Dpf,f(Cpg)=Cphf(\mathscr{D}^pg) = \mathscr{D}^pf, f(\mathscr{C}^pg) = \mathscr{C}^ph.

If a and b are submodules of g, it follows immediately that

f([a,b])=[f(a),f(b)]. f([a, b]) = [f(a), f(b)].
The proposition is then immediate by induction on pp.

Corollary

Let g be a Lie algebra and a an ideal of g. For the Lie algebra g/ag/a to be commutative, it is necessary and sufficient that a⊃Dga \supset \mathscr{D}g.

To say that g/ag/a is commutative amounts to saying that D(g/a)={0}\mathscr{D}(g/a) = \{0\}. But D(g/a)\mathscr{D}(g/a) is, by Proposition 4, the canonical image of Dg\mathscr{D}g in g/ag/a.

6. Upper central series

Let g be a Lie algebra and P a subset of g. The centralizer of P in g is the set of elements of g which are permutable with those of P. This centralizer is the intersection of the kernels of the ad yy, where yy runs through P; it is therefore a subalgebra of g.

Proposition 5

Let g be a Lie algebra and a an ideal (resp. a characteristic ideal) of g. The centralizer a′a' of a in g is an ideal (resp. a characteristic ideal) of g.

Let D be an inner derivation (resp. a derivation) of g. If x∈a′x \in a' and y∈ay \in a, then

[Dx,y]=D([x,y])−[x,Dy]=0; [Dx, y] = D([x, y]) - [x, Dy] = 0;
hence Dx∈a′Dx \in a'. Hence the proposition.

Let gg be a Lie algebra. The centralizer of gg in gg is called the centre of gg, that is the characteristic ideal of x∈gx \in g such that [x,y]=0[x, y] = 0 for all y∈gy \in g. The centre of gg is the kernel of the homomorphism x↦ad xx \mapsto \mathrm{ad}\, x.

The upper central series of gg is the increasing sequence C0g,C1g,…\mathscr{C}_0 g, \mathscr{C}_1 g, \ldots of characteristic ideals of gg defined inductively as follows: (1) C0g={0}\mathscr{C}_0 g = \{0\}; (2) Cp+1g\mathscr{C}_{p+1} g is the inverse image under the canonical mapping of gg onto g/Cpgg / \mathscr{C}_p g of the centre of g/Cpgg / \mathscr{C}_p g The ideal C1g\mathscr{C}_1 g is the centre of gg.

7. Extensions

Definition 5

Let aa and bb be two Lie algebras over KK. An extension of bb by aa is a sequence:

a→λg→μb a \xrightarrow{\lambda} g \xrightarrow{\mu} b

where gg is a Lie algebra over KK, μ\mu a surjective homomorphism of gg onto bb and λ\lambda an injective homomorphism of aa onto the kernel of μ\mu.

The kernel nn of μ\mu is called the kernel of the extension. The homomorphism λ\lambda is an isomorphism of aa onto nn and the homomorphism μ\mu defines an isomorphism of g/ng / n onto bb when passing to the quotient. By an abuse of language, gg is also called an extension of bb by aa.

Two extensions:

a→λg→μb,a→λ′g′→μ′b a \xrightarrow{\lambda} g \xrightarrow{\mu} b, \quad a \xrightarrow{\lambda'} g' \xrightarrow{\mu'} b

are said to be equivalent if there exists a homomorphism ff of gg into g′g' such that the following diagram:

a→λg→μbf↓g′→μ′ba→λ′g′→μ′b \begin{array}{ccccc} a & \xrightarrow{\lambda} & g & \xrightarrow{\mu} & b \\ & & f \downarrow & & \\ & & g' & \xrightarrow{\mu'} & b \\ a & \xrightarrow{\lambda'} & g' & \xrightarrow{\mu'} & b \end{array}

is commutative (that is such that f∘λ=λ′,μ′∘f=μf \circ \lambda = \lambda', \mu' \circ f = \mu). We show that such a homomorphism is necessarily bijective. First ff is injective. For if x∈gx \in g is such that f(x)=0f(x) = 0, then μ(x)=μ′(f(x))=0\mu(x) = \mu'(f(x)) = 0 and hence x=λ(y)x = \lambda(y) for some y∈ay \in a; then λ′(y)=f(λ(y))=f(x)=0\lambda'(y) = f(\lambda(y)) = f(x) = 0, hence y=0y = 0 and hence x=0x = 0. On the other hand, ff is surjective. For μ′∘f=μ\mu' \circ f = \mu is surjective and hence f(g)+λ′(a)=g′f(g) + \lambda'(a) = g'; on the other hand f(g)⊃f(λ(a))=λ′(a)f(g) \supset f(\lambda(a)) = \lambda'(a).

It follows from this that the relation just defined between two extensions of bb by aa is an equivalence relation.

Proposition 6

Let

a→λg→μb a \xrightarrow{\lambda} g \xrightarrow{\mu} b

be an extension of bb by aa and nn its kernel.

(a) If there exists a subalgebra m of g supplementary to n in g, the restriction of μ to m is an isomorphism of m onto b. If ν denotes the inverse isomorphism of this restriction, ν is a homomorphism of b into g and μ ∘ ν is the identity automorphism of b.

(b) Conversely, if there exists a homomorphism ν of b into g such that μ ∘ ν is the identity automorphism of b, then ν(b) is a supplementary subalgebra of n in g.

The assertions of (a) are immediate. On the other hand, let ν be a homomorphism of b into g such that μ ∘ ν is the identity automorphism of b. Then ν(b) is a subalgebra of g and g is the direct sum of ν(b) and μ−1(0)=n\mu^{-1}(0) = n (Algebra, Chapter VIII, § 1, no. 1).

Definition 6

Let

a→λg→μb a \xrightarrow{\lambda} g \xrightarrow{\mu} b

be an extension of b by a and n its kernel. This extension is called inessential (resp. trivial) if there exists a subalgebra (resp. an ideal) of g supplementary to n in g. This extension is called central if n is contained in the centre of g.

If the extension is trivial, let m be an ideal of g supplementary to n in g. Then (cf. no. 1) g is canonically identified with the Lie algebra m × n and hence with the Lie algebra a × b. Conversely, let a and b be two Lie algebras; then a × b is a trivial extension of a by b.

An inessential central extension is trivial. For let g be a Lie algebra, n an ideal of g contained in the centre of g and m a subalgebra of g supplementary to n in g. Then [m, g] = [m, m] + [m, n] = [m, m] ⊂ m and hence m is an ideal of g.

8. Semi-direct products

Let a and b be two Lie algebras over K. It is not easy to construct all the extensions of b by a. But we shall describe quite simply all the inessential extensions of b by a.

Let g be an inessential extension of b by a. We identify a with an ideal of g, b with a subalgebra of g supplementary to a and the module g with the module a × b. For all b∈bb \in b, let ϕb\phi_b be the restriction to a of adg b\mathrm{ad}_g\ b; this is a derivation of a and the mapping b↦ϕbb \mapsto \phi_b is a homomorphism of b into the Lie algebra of derivations of a. On the other hand, for a,a′a, a' in a and b,b′b, b' in b, we have:

[(a,b),(a′,b′)]=[a+b,a′+b′]=[a,a′]+[a,b′]+[b,a′]+[b,b′]=([a,a′]+ϕba′−ϕb′a,[b,b′]). [(a, b), (a', b')] = [a + b, a' + b'] = [a, a'] + [a, b'] + [b, a'] + [b, b'] = ([a, a'] + \phi_b a' - \phi_{b'} a, [b, b']).

Conversely, let a and b be Lie algebras over K and b↦ϕbb \mapsto \phi_b a homomorphism of b into the Lie algebra of derivations of a. On the product g of the K-modules a and b we define the bracket of two elements by writing:

[(a,b),(a′,b′)]=([a,a′]+ϕba′−ϕb′a,[b,b′]) [(a, b), (a', b')] = ([a, a'] + \phi_b a' - \phi_{b'} a, [b, b'])

for all a,a′a, a' in aa, b,b′b, b' in bb. It is immediate that this bracket is an alternating bilinear function of (a,b),(a′,b′)(a, b), (a', b'); we show that, given 3 elements (a,b),(a′,b′),(a′′,b′′)(a, b), (a', b'), (a'', b'') of a×ba \times b:

(7)

[(a,b),[(a′,b′),(a′′,b′′)]]+[(a′,b′),[(a′′,b′′),(a,b)]]+[(a′′,b′′),[(a,b),(a′,b′)]]=0. [(a, b), [(a', b'), (a'', b'')]] + [(a', b'), [(a'', b''), (a, b)]] \\ + [(a'', b''), [(a, b), (a', b')]] = 0.

As the left hand side of (7) is an alternating trilinear function of (a,b),(a′,b′),(a′′,b′′)(a, b), (a', b'), (a'', b''), it suffices to make the verification when this system of elements takes one of the following forms:

(8) (a,0),(a′,0),(a′′,0)(a, 0), (a', 0), (a'', 0)

(9) (a,0),(a′,0),(0,b′′)(a, 0), (a', 0), (0, b'')

(10) (a,0),(0,b′),(0,b′′)(a, 0), (0, b'), (0, b'')

(11) (0,b),(0,b′),(0,b′′)(0, b), (0, b'), (0, b'').

In cases (8) and (11), relation (7) is an immediate consequence of the Jacobi identity in aa and bb. In case (9), we have

[(a,0),[(a′,0),(0,b′′)]]=[(a,0),(−ϕb′′a′,0)]=(−[a,ϕb′′a′],0) [(a, 0), [(a', 0), (0, b'')]] = [(a, 0), (-\phi_{b''}a', 0)] = (-[a, \phi_{b''}a'], 0)
[(a′,0),[(0,b′′),(a,0)]]=[(a′,0),(ϕb′′a,0)]=([a′,ϕb′′a],0) [(a', 0), [(0, b''), (a, 0)]] = [(a', 0), (\phi_{b''}a, 0)] = ([a', \phi_{b''}a], 0)
[(0,b′′),[(a,0),(a′,0)]]=[(0,b′′),([a,a′],0)]=(ϕb′′([a,a′]),0) [(0, b''), [(a, 0), (a', 0)]] = [(0, b''), ([a, a'], 0)] = (\phi_{b''}([a, a']), 0)

and relation (7) follows from the equation:

ϕb′′([a,a′])=[ϕb′′a,a′]+[a,ϕb′′a′]. \phi_{b''}([a, a']) = [\phi_{b''}a, a'] + [a, \phi_{b''}a'].

In case (10), we have:

[(a,0),[(0,b′),(0,b′′)]]=[(a,0),(0,[b′,b′′])]=(−ϕ[b′,b′′]a,0) [(a, 0), [(0, b'), (0, b'')]] = [(a, 0), (0, [b', b''])] = (-\phi_{[b', b'']}a, 0)
[(0,b′),[(0,b′′),(a,0)]]=[(0,b′),(ϕb′′a,0)]=(ϕb′ϕb′′a,0) [(0, b'), [(0, b''), (a, 0)]] = [(0, b'), (\phi_{b''}a, 0)] = (\phi_{b'}\phi_{b''}a, 0)
[(0,b′′),[(a,0),(0,b′)]]=[(0,b′′),(−ϕb′a,0)]=(−ϕb′′ϕb′a,0) [(0, b''), [(a, 0), (0, b')]] = [(0, b''), (-\phi_{b'}a, 0)] = (-\phi_{b''}\phi_{b'}a, 0)

and relation (7) follows from the equation:

ϕ[b′,b′′]=ϕb′ϕb′′−ϕb′′ϕb′. \phi_{[b', b'']} = \phi_{b'}\phi_{b''} - \phi_{b''}\phi_{b'}.

Hence a Lie algebra structure has been defined on gg. The mapping (a,b)↦b(a, b) \mapsto b of gg onto bb is a homomorphism μ\mu whose kernel nn is the ideal of elements of gg of the form (a,0)(a, 0). The mapping a↦(a,0)a \mapsto (a, 0) is an isomorphism λ\lambda of aa onto nn. Hence:

(12)

a→λg→μb a \xrightarrow{\lambda} g \xrightarrow{\mu} b

is an extension of bb by aa of kernel nn, which is said to be canonically defined by a,b,ϕa, b, \phi. The mapping b↦(0,b)b \mapsto (0, b) is an isomorphism ν\nu of bb onto a subalgebra of gg supplementary to nn in gg; hence the extension is inessential.

If aa is identified with nn under λ\lambda and bb with v(b)v(b) under vv, then, for a∈aa \in a and b∈bb \in b:

(ad b).a=[(0,b),(a,0)]=(ϕba,0)=ϕba. (\mathrm{ad}\ b).a = [(0, b), (a, 0)] = (\phi_b a, 0) = \phi_b a.

When ϕ=0\phi = 0, gg is the product Lie algebra of bb and aa. In the general case, gg is called the semi-direct product of bb by aa (corresponding to the homomorphism b↦ϕbb \mapsto \phi_b of bb into the Lie algebra of derivations of aa).

We have therefore established the following proposition:

Proposition 7

Let aa and bb be two Lie algebras over KK,

a→λg→μb a \xrightarrow{\lambda} g \xrightarrow{\mu} b

an inessential extension of bb by aa, ν\nu an isomorphism of bb onto a subalgebra of gg such that μ∘ν\mu \circ \nu is the identity automorphism of bb and ϕ\phi the corresponding homomorphism of bb into the Lie algebra of derivations of aa. Let

a→λ0g0→μ0b a \xrightarrow{\lambda_0} g_0 \xrightarrow{\mu_0} b

be the inessential extension of bb by aa canonically defined by ϕ\phi. Then the mapping (a,b)↦λ(a)+ν(b)(a, b) \mapsto \lambda(a) + \nu(b) is an isomorphism ff of g0g_0 onto gg and the following diagram

a→λ0g0→μ0b↘f↓↗μ0g↙i↘μ \begin{array}{ccccc} & & \\ a & \xrightarrow{\lambda_0} & g_0 & \xrightarrow{\mu_0} & b \\ & \searrow f & \downarrow & \nearrow \mu_0 \\ & & g & & \\ & \swarrow i & & \searrow \mu \\ & & & & \end{array}

is commutative, so that the two extensions are equivalent.

Example 1

Let gg be a Lie algebra over KK and DD a derivation of gg. Let hh be the commutative Lie algebra KK. The mapping λ↦λD(λ∈K)\lambda \mapsto \lambda D (\lambda \in K) is a homomorphism of hh into the Lie algebra of derivations of gg. We form the corresponding semi-direct product tt of hh by gg. Let x0x_0 be the element (0,1)(0, 1) of tt. For all x∈gx \in g, Dx=[x0,x]Dx = [x_0, x].

Example 2

Let gg be a Lie algebra over KK, MM a KK-module and ρ\rho a homomorphism of gg into gl(M)\mathfrak{gl}(M). If MM is considered as a commutative Lie algebra, the Lie algebra of derivations of MM is gl(M)\mathfrak{gl}(M). We can therefore form the semi-direct product hh of gg by MM corresponding to ρ\rho.

In particular, let g=gl(M)g = \mathfrak{gl}(M) and ρ\rho be the identity mapping of gl(M)\mathfrak{gl}(M). The semi-direct product of gg by MM is then denoted by af(M)\mathfrak{af}(M) (or af(n,K)\mathfrak{af}(n, K) if M=KnM = K^n). An element of af(M)\mathfrak{af}(M) is an ordered pair (m,u)(m, u), where m∈M,u∈gl(M)m \in M, u \in \mathfrak{gl}(M); and the bracket is defined by

[(m,u),(m′,u′)]=(u(m′)−u′(m),[u,u′]). [(m, u), (m', u')] = (u(m') - u'(m), [u, u']).

When M is a finite-dimensional vector space over R\mathbf{R}, af(M)\mathfrak{af}(M) is canonically identified with the Lie algebra of the affine group of M.

Let tt be a Lie algebra over K. A linear mapping θ\theta of tt into af(M)\mathfrak{af}(M) can be written x↦((ζ(x),η(x)))x \mapsto ((\zeta(x), \eta(x))), where ζ\zeta is a linear mapping of tt into MM and η\eta a linear mapping of tt into gl(M)gl(M). We examine the conditions that ζ\zeta and η\eta must satisfy for θ\theta to be a homomorphism. For x∈t,y∈tx \in t, y \in t, we must have

θ([x,y])=[θ(x),θ(y)] \theta([x, y]) = [\theta(x), \theta(y)]

that is

(ζ([x,y]),η([x,y]))=[(ζ(x),η(x)),(ζ(y),η(y))]=(η(x)⋅ζ(y)−η(y)⋅ζ(x),[η(x),η(y)]). (\zeta([x, y]), \eta([x, y])) = [(\zeta(x), \eta(x)), (\zeta(y), \eta(y))] \\ = (\eta(x) \cdot \zeta(y) - \eta(y) \cdot \zeta(x), [\eta(x), \eta(y)]).

Hence for θ\theta to be a homomorphism of tt into af(M)\mathfrak{af}(M), it is necessary and sufficient that η\eta be a homomorphism of tt into gl(M)gl(M) and that ζ\zeta satisfy the relation:

(13)

ζ([x,y])=η(x)⋅ζ(y)−η(y)⋅ζ(x). \zeta([x, y]) = \eta(x) \cdot \zeta(y) - \eta(y) \cdot \zeta(x).

Let N be the K-module M×KM \times K. We take tt to be the subalgebra of gl(N)gl(N) consisting of the w∈gl(N)w \in gl(N) such that w(N)⊂Mw(N) \subset M. For all w∈tw \in t, let η(w)∈gl(M)\eta(w) \in gl(M) be the restriction of ww to MM and let ζ(w)=w(0,1)∈M\zeta(w) = w(0, 1) \in M. For w1∈t,w2∈tw_1 \in t, w_2 \in t,

ζ([w1,w2])=w1(ζ(w2))−w2(ζ(w1))=η(w1)⋅ζ(w2)−η(w2)⋅ζ(w1). \zeta([w_1, w_2]) = w_1(\zeta(w_2)) - w_2(\zeta(w_1)) = \eta(w_1) \cdot \zeta(w_2) - \eta(w_2) \cdot \zeta(w_1).

Hence the mapping w↦(ζ(w)),η(w))w \mapsto (\zeta(w)), \eta(w)) is a homomorphism θ\theta of tt into af(M)\mathfrak{af}(M). Clearly θ\theta is bijective. Let ϕ=θ−1\phi = \theta^{-1}. If (m,u)∈af(M)(m, u) \in \mathfrak{af}(M), ϕ(m,u)\phi(m, u) is the element ww of tt defined by

w(m′,λ)=(u(m′)+λm,0). w(m', \lambda) = (u(m') + \lambda m, 0).

af(M)\mathfrak{af}(M) is often identified with the subalgebra tt of gl(N)gl(N) under the isomorphism ϕ\phi.

When M is a finite-dimensional vector space over R\mathbf{R}, the homomorphism ϕ\phi of af(M)\mathfrak{af}(M) into gl(N)gl(N) corresponds to a canonical homomorphism ψ\psi of the affine group A of M into the group GL(N)\mathbf{GL}(N); if a∈A,ψ(a)a \in A, \psi(a) is the unique element gg of GL(N)\mathbf{GL}(N) such that g(m,1)=(a(m),1)g(m, 1) = (a(m), 1) for all m∈Mm \in M. This homomorphism is injective and ψ(A)\psi(A) is the set of automorphisms of N which leave invariant all the linear varieties of N parallel to M.

9. Change of base ring

Let K0K_0 be a commutative ring with unit element and ρ\rho a homomorphism of K0K_0 into K mapping unit element to unit element. Let gg be a Lie algebra over K. Let g′g' be the algebra obtained by considering gg as an algebra over K0K_0 by means of ρ\rho (cf. no. 1). Then g′g' is a Lie algebra. The subalgebras (resp. ideals) of gg are subalgebras (resp. ideals) of g′g'. If aa and bb are submodules of gg, the bracket [a,b][a, b] is the same in gg and in g′g'; for [a,b][a, b] is the set of elements of the form

∑i=1n[xi,yi] \sum_{i=1}^n [x_i, y_i]

where xi∈a,yi∈bx_i \in a, y_i \in b. It follows that Dpg=Dpg′,Cpg=Cpg′\mathscr{D}^p g = \mathscr{D}^p g', \mathscr{C}^p g = \mathscr{C}^p g' for all pp.

The centralizer of a subset is the same in gg and g′g'. Hence Cpg=Cpg′\mathscr{C}_p g = \mathscr{C}_p g' for all pp.

Let K1K_1 be a commutative ring with unit element and σ\sigma a homomorphism of KK into K1K_1 mapping unit element to unit element. Let gg be a Lie algebra over KK. Let g(K1)g_{(K_1)} be the algebra over K1K_1 derived from gg by extending the base ring (cf. no. 1). Then g(K1)g_{(K_1)} is a Lie algebra. If aa is a subalgebra (resp. an ideal) of gg, the canonical image of a(K1)a_{(K_1)} in g(K1)g_{(K_1)} is a subalgebra (resp. an ideal) of g(K1)g_{(K_1)}. If aa and bb are submodules of gg, the canonical image in g(K1)g_{(K_1)} of [a,b](K1)[a, b]_{(K_1)} is equal to the bracket of the canonical images of a(K1)a_{(K_1)} and b(K1)b_{(K_1)}. It follows that Dp(g(K1))\mathscr{D}^p(g_{(K_1)}) is the canonical image of (Dpg)(K1)(\mathscr{D}^p g)_{(K_1)} and that Cp(g(K1))\mathscr{C}^p(g_{(K_1)}) is the canonical image of Cp(g(K1))\mathscr{C}^p(g_{(K_1)}).

If KK is a field, K1K_1 an extension field of KK and σ\sigma the canonical injection of KK into K1K_1, then with the usual identifications we have

[a,b](K1)=[a(K1),b(K1)],Dp(g(K1))=(Dpg)(K1), [a, b]_{(K_1)} = [a_{(K_1)}, b_{(K_1)}], \quad \mathscr{D}^p(g_{(K_1)}) = (\mathscr{D}^p g)_{(K_1)},
Cp(g(K1))=(Cpg)(K1). \mathscr{C}^p(g_{(K_1)}) = (\mathscr{C}^p g)_{(K_1)}.

These results are completed in § 2, no. 9.

If MM is a finite-dimensional vector space over the field KK, M(K1)M_{(K_1)} is a finite-dimensional vector space over K1K_1 and the associative algebra L(M(K1))\mathscr{L}(M_{(K_1)}) is canonically identified with the associative algebra L(M)(K1)\mathscr{L}(M)_{(K_1)}. Hence the Lie algebra gl(M(K1))gl(M_{(K_1)}) is canonically identified with the Lie algebra gl(M)(K1)gl(M)_{(K_1)}.

Exercises

See the exercises for § 1.

Transcribed from the printed volume. Not translated.