Bourbaki

§ 3. Passage from a Lie group to its Lie algebra

1. Convolution of point distributions on a Lie group

Definition 1

Let GG be a Lie group, gg and g′g' two points of GG and let t∈Tg(∞)(G)t \in T_g^{(\infty)}(G) t′∈Tg′(∞)(G)t' \in T_{g'}^{(\infty)}(G) be two point distributions at gg and g′g' on GG (Differentiable and Analytic Manifolds, R, 13.2.1). The convolution product of tt and t′t', denoted by t∗t′t * t', is the image of t⊗t′t \otimes t' under the mapping (h,h′)↦hh′(h, h') \mapsto hh' of G×GG \times G into GG (Differentiable and Analytic Manifolds, R, 13.2.3).

Proposition 1

(i) *If t∈Tg(s)(G)t \in T_g^{(s)}(G) and t′∈Tg′(s′)(G)t' \in T_{g'}^{(s')}(G), then t∗t′∈Tgg′(s+s′)(G)t * t' \in T_{gg'}^{(s+s')}(G).

(ii) If tt or tt has no constant term, t∗t′t * t' has no constant term.

(iii) εg∗εg′=εgg′\varepsilon_g * \varepsilon_{g'} = \varepsilon_{gg'}.

(iv) Let t∈Tg(s)(G)t \in T_g^{(s)}(G), t′∈Tg′(s′)(G)t' \in T_{g'}^{(s')}(G) and let ff be a function of class Cs+s′C^{s+s'} in an open neighbourhood of gg′gg' with values in a Hausdorff polynormed space. Then

⟨t∗t′,f⟩=⟨t′,h′↦⟨t,h↦f(hh′)⟩⟩=⟨t,h↦⟨t′,h′↦f(hh′)⟩⟩. \langle t * t', f \rangle = \langle t', h' \mapsto \langle t, h \mapsto f(hh') \rangle \rangle \\ = \langle t, h \mapsto \langle t', h' \mapsto f(hh') \rangle \rangle.

This follows from Differentiable and Analytic Manifolds, R, 13.4.1, 13.2.3 and 13.4.4.

Suppose that K = \mathbf{R} or \mathbf{C} and that G is finite-dimensional. Then G is locally compact. If t, t' are point measures, the definition of t \* t' agrees with that of Integration, Chapter VIII, § 1. We shall see later that the convolution product of measures and that of point distributions are two special cases of the convolution product of distributions which are not necessarily point distributions.

Let \mathscr{T}^{(\infty)}(G) be the direct sum of the T_g^{(\infty)}(G) for g \in G (cf. Differentiable and Analytic Manifolds, R, 13.6.1). We define the convolution product in \mathscr{T}^{(\infty)}(G) as the bilinear mapping of \mathscr{T}^{(\infty)}(G) \times \mathscr{T}^{(\infty)}(G) into \mathscr{T}^{(\infty)}(G) extending the convolution product of Definition 1. We also denote it by . Thus \mathscr{T}^{(\infty)}(G) has an algebra structure filtered by the \mathscr{T}^{(s)}(G). The subalgebra \mathscr{T}^{(0)}(G) = \bigoplus{g \in G} T_g^{(0)}(G) is identified with the algebra K^{(G)} of the group G over K.

Proposition 2

The algebra \mathscr{T}^{(\infty)}(G) is associative. It is commutative if and only if G is commutative.

Let t \in \mathscr{T}^{(\infty)}(G), t' \in \mathscr{T}^{(\infty)}(G), t'' \in \mathscr{T}^{(\infty)}(G). Then t \* (t' \* t'') is the image of t \otimes t' \otimes t'' under the mapping (g, g', g'') \mapsto g(g'g'') of G \times G \times G into G and (t \* t') \* t'' is the image of t \otimes t' \otimes t'' under the mapping (g, g', g'') \mapsto (gg')g'' of G \times G \times G into G. Hence (t \* t') \* t'' = t \* (t' \* t''). It is seen similarly that, if G is commutative, t \* t' = t' \* t. If the convolution product is commutative, G is commutative by Proposition 1 (iii).

Proposition 3

If t \in \mathscr{T}^{(\infty)}(G) and g \in G, then γ(g)∗t=εg∗t,δ(g)∗t=t∗εg−1\gamma(g)_* t = \varepsilon_g * t, \delta(g)_* t = t * \varepsilon_{g^{-1}}, (Int g)_* t = εg∗t∗εg−1\varepsilon_g * t * \varepsilon_{g^{-1}}. In particular, εe\varepsilon_e is the unit element of \mathscr{T}^{(\infty)}(G).

Consider the diagram

G→ϕG×G→ψG \begin{array}{ccccc} G & \xrightarrow{\phi} & G \times G & \xrightarrow{\psi} & G \\ \end{array}

where ϕ\phi is the mapping h↦(g,h)h \mapsto (g, h) and ψ\psi is the mapping (h′,h)↦h′h(h', h) \mapsto h'h. Then γ(g)=ψ∘ϕ\gamma(g) = \psi \circ \phi and hence γ(g)∗t=ψ∗(ϕ∗(t))\gamma(g)_* t = \psi_*(\phi_*(t)). But ϕ∗(t)=εg⊗t\phi_*(t) = \varepsilon_g \otimes t and hence ψ∗(ϕ∗(t))=εg∗t\psi_*(\phi_*(t)) = \varepsilon_g * t. The argument is similar for δ(g)∗t\delta(g)_* t. Finally,

Int⁡g=γ(g)∘δ(g) \operatorname{Int} g = \gamma(g) \circ \delta(g)

and hence (Int⁡g)∗=γ(g)∗∘δ(g)∗(\operatorname{Int} g)_* = \gamma(g)_* \circ \delta(g)_*.

It is therefore seen that, for t∈T(G)t \in T(G), εg∗t\varepsilon_g * t and t∗εgt * \varepsilon_g are equal to gtgt and tgtg calculated in the group T(G) (§ 2, no. 2). But it should be noted that, for t,t′t, t' in T(G), the product tt′tt' in the sense of § 2 is in general different from t∗t′t * t'.

Definition 2

Let G be a Lie group. The subalgebra of T(∞)(G)\mathscr{T}^{(\infty)}(G) consisting of the distributions with support contained in e is denoted by U(G)U(G).

This algebra is filtered by the subspaces

Us(G)=U(G)∩T(s)(G)=Te(s)(G). U_s(G) = U(G) \cap \mathscr{T}^{(s)}(G) = T_e^{(s)}(G).
We write U+(G)=Te(∞)+(G)U^+(G) = T_e^{(\infty)+}(G), Us+(G)=U+(G)∩Us(G)U_s^+(G) = U^+(G) \cap U_s(G) (cf. Differentiable and Analytic Manifolds, R, 13.2.1). Recall that U0(G)U_0(G) is identified with K and U1+(G)U_1^+(G) with the tangent space Te(G)T_e(G). In U(G)U(G), U+(G)U^+(G) is a two-sided ideal supplementary to U0(G)U_0(G).

Example

Let E be a complete normable space considered as a Lie group. Then the vector space U(E)U(E) is canonically identified with the vector space TS(E) (Differentiable and Analytic Manifolds, R, 13.2.4). Let m:E×E→Em : E \times E \to E be addition on E. Then

m∗:TS(E×E)→TS(E) m_* : TS(E \times E) \to TS(E)
is equal to TS(m) (Differentiable and Analytic Manifolds, R, 13.2.4). For t,t′t, t' in U(E)=TS(E)U(E) = TS(E), the image t∗t′t * t' of the symmetric tensor product t⊗t′t \otimes t' under m∗m_* is therefore TS(m)(t⊗t′t \otimes t'). By Algebra, Chapter IV, § 5, no. 6, Proposition 7, this image is just the product tt′tt' in the algebra TS(E). Thus the algebra U(E)U(E) is identified with the algebra TS(E).

Proposition 4

Consider the bilinear mapping (u,v)↦u∗v(u, v) \mapsto u * v (resp. (u,v)↦v∗u(u, v) \mapsto v * u) of U(G)⊗K(G)U(G) \otimes K^{(G)} into T(∞)(G)\mathscr{T}^{(\infty)}(G). The corresponding linear mapping of U(G)⊗K(G)U(G) \otimes K^{(G)} into T(∞)(G)\mathscr{T}^{(\infty)}(G) is a vector space isomorphism.

K(G)K^{(G)} is the direct sum of the KexK_{e_x} for x∈Gx \in G. On the other hand, the mapping u↦u∗εgu \mapsto u * \varepsilon_g (resp. u↦εg∗uu \mapsto \varepsilon_g * u) is an isomorphism of the vector space U(G)=Te(∞)(G)U(G) = \mathscr{T}_e^{(\infty)}(G) onto the vector space Tg(∞)(G)\mathscr{T}_g^{(\infty)}(G) by Proposition 3. Finally, T(∞)(G)\mathscr{T}^{(\infty)}(G) is the direct sum of the Tg(∞)(G)T_g^{(\infty)}(G) for g∈Gg \in G.

Let X be a manifold of class CrC^r (r≥∞r \geq \infty) and x∈Xx \in X. We have defined (Differentiable and Analytic Manifolds, R, 13.3.1) a canonical filtration on the vector space Tx(∞)(X)\mathscr{T}_x^{(\infty)}(X) and a canonical isomorphism iX,xi_{X,x} of the associated graded vector space onto the graded vector space TS(T_x(X)). In particular, let Te(G)=LT_e(G) = L; then iG,ei_{G,e} is an isomorphism of the graded vector space gr U(G) onto the graded vector space TS(L). But U(G) is a filtered algebra, from which we obtain a graded algebra structure on gr U(G).

Proposition 5

The isomorphism iG,e:gr U(G)→TS(L)i_{G,e} : \mathrm{gr}\ U(G) \to \mathrm{TS}(L) is an algebra isomorphism.

Let pp be the mapping (t,t′)↦t⊗t′(t, t') \mapsto t \otimes t' of U(G)×U(G)U(G) \times U(G) into U(G×G)U(G \times G). Let c be the mapping (t,t′)↦t∗t′(t, t') \mapsto t * t' of U(G)×U(G)U(G) \times U(G) into U(G)U(G). Let m be the mapping (g,g′)↦gg′(g, g') \mapsto gg' of G×GG \times G into G. Then by Definition 1

c=m∗∘p. c = m_* \circ p.

Consider the diagram

gr U(G)×gr U(G)→gr(p)gr U(G×G)↓iG,e×iG,e↓iG×G,eTS(L)×TS(L)→qTS(L×L)→TS(T(m))TS(L) \begin{array}{ccc} \mathrm{gr}\,\mathrm{U}(G) \times \mathrm{gr}\,\mathrm{U}(G) & \xrightarrow{\mathrm{gr}(p)} & \mathrm{gr}\,\mathrm{U}(G \times G) \\ \downarrow i_{G,e} \times i_{G,e} & & \downarrow i_{G \times G,e} \\ \mathrm{TS}(L) \times \mathrm{TS}(L) & \xrightarrow{q} & \mathrm{TS}(L \times L) \\ & & \xrightarrow{\mathrm{TS}(T(m))} \mathrm{TS}(L) \end{array}
where qq is the mapping derived from the canonical isomorphism of TS(L)×TS(L)\mathrm{TS}(L) \times \mathrm{TS}(L) onto TS(L×L)\mathrm{TS}(L \times L). By Differentiable and Analytic Manifolds, R, 13.4.6 and 13.3.5, the two squares of the diagram are commutative. Hence by (1) the diagram
gr U(G)×gr U(G)→gr(c)gr U(G)↓iG,e×iG,e↓iG,eTS(L)×TS(L)→TS(T(m))∘qTS(L) \begin{array}{ccc} \mathrm{gr}\,\mathrm{U}(G) \times \mathrm{gr}\,\mathrm{U}(G) & \xrightarrow{\mathrm{gr}(c)} & \mathrm{gr}\,\mathrm{U}(G) \\ \downarrow i_{G,e} \times i_{G,e} & & \downarrow i_{G,e} \\ \mathrm{TS}(L) \times \mathrm{TS}(L) & \xrightarrow{\mathrm{TS}(T(m)) \circ q} & \mathrm{TS}(L) \end{array}
is commutative. Now T(m):L×L→LT(m): L \times L \to L maps (x,y)(x, y) to x+yx + y (§ 2, no. 1, Proposition 2 (ii)). By Algebra, Chapter IV, § 5, no. 6, Proposition 7, TS(T(m))∘q\mathrm{TS}(T(m)) \circ q is therefore the multiplication of the algebra TS(L)\mathrm{TS}(L).

2. Functioral properties

Proposition 6

Let G,HG, H be Lie groups and ϕ\phi a morphism of GG into HH. For t,t′t, t' in T(∞)(G)\mathscr{T}^{(\infty)}(G), ϕ∗(t∗t′)=ϕ∗(t)∗ϕ∗(t′)\phi_*(t * t') = \phi_*(t) * \phi_*(t').

Consider the diagram

G×G→mGϕ×ϕ↓↓ϕH×H→nH \begin{array}{ccc} G \times G & \xrightarrow{m} & G \\ \phi \times \phi \downarrow & & \downarrow \phi \\ H \times H & \xrightarrow{n} & H \end{array}
where m(g,g′)=gg′m(g, g') = gg', n(h,h′)=hh′n(h, h') = hh'. This diagram is commutative. Hence
ϕ∗(t∗t′)=ϕ∗(m∗(t⊗t′))=n∗((ϕ×ϕ)∗(t⊗t′))=n∗(ϕ∗(t)⊗ϕ∗(t′))=ϕ∗(t)∗ϕ∗(t′). \begin{align*} \phi_*(t * t') &= \phi_*(m_*(t \otimes t')) = n_*((\phi \times \phi)_*(t \otimes t')) \\ &= n_*(\phi_*(t) \otimes \phi_*(t')) = \phi_*(t) * \phi_*(t'). \end{align*}

The Lie groups GG and G∨G^\vee have the same underlying manifold and hence the vector spaces T(∞)(G)\mathscr{T}^{(\infty)}(G) and T(∞)(G∨)\mathscr{T}^{(\infty)}(G^\vee) are the same. Let θ\theta be the mapping g↦g−1g \mapsto g^{-1}, which is an isomorphism of the Lie group GG onto the Lie group G∨G^\vee. Then θ∗\theta^* is an automorphism of the vector space T(∞)(G)\mathscr{T}^{(\infty)}(G), which automorphism we denote by t↦t∨t \mapsto t^\vee. Then (εg)∨=εg−1(\varepsilon_g)^\vee = \varepsilon_{g^{-1}}. If t∈Te(G)t \in T_e(G), then

t∨=−t(§2,Proposition 2). t^\vee = -t \quad (§ 2, \text{Proposition 2}).

Example

Suppose that GG is the Lie group defined by a complete normable space EE. Then U(G)\mathrm{U}(G) is identified with TS(E)\mathrm{TS}(E) and the restriction θ∗\theta_* to U(G)\mathrm{U}(G) is identified with TS(Te(θ))\mathrm{TS}(T_e(\theta)) (Differentiable and Analytic Manifolds, R, 13.2.4). Therefore, if t∈TSs(E)t \in \mathrm{TS}^s(E), t∨=(−1)stt^\vee = (-1)^s t.

Proposition 7

Let G be a Lie group. Let t, t' be in T(∞)(G)\mathscr{T}^{(\infty)}(G).

(i) The product t∗t′t * t' calculated relative to G∨G^\vee is equal to the product t′∗tt' * t calculated relative to G.

(ii) (t∗t′)∨=t′∨∗t∨(t * t')^\vee = {t'}^\vee * t^\vee.

Consider the diagram

(G1×G2)×(G1×G2)→mG1×G2↓n↑p1×p2(G1×G1)×(G2×G2) \begin{array}{ccc} (G_1 \times G_2) \times (G_1 \times G_2) & \xrightarrow{m} & G_1 \times G_2 \\ \downarrow n & & \uparrow p_1 \times p_2 \\ (G_1 \times G_1) \times (G_2 \times G_2) \end{array}

where s(g,g′)=(g′,g)s(g, g') = (g', g), m(g,g′)=gg′m(g, g') = gg', n(g,g′)=g′gn(g, g') = g'g for all g,g′g, g' in G. This diagram is commutative. Hence n∗(t⊗t′)=m∗(s∗(t⊗t′))=m∗(t′⊗t)n_*(t \otimes t') = m_*(s_*(t \otimes t')) = m_*(t' \otimes t). This equality is precisely (i). Assertion (ii) follows from (i) and Proposition 6.

Proposition 8

Let G, H be Lie groups and ϕ\phi a morphism of G into H. If t∈T(∞)(G)t \in \mathscr{T}^{(\infty)}(G), then ϕ∗(t∨)=(ϕ∗(t))∨\phi_*(t^\vee) = (\phi_*(t))^\vee.

Let θ\theta (resp. θ′\theta') be the mapping g↦g−1g \mapsto g^{-1} of G into G (resp. of H into H). Then ϕ∘θ=θ′∘ϕ\phi \circ \theta = \theta' \circ \phi, whence ϕ∗(θ∗(t))=θ∗′(ϕ∗(t))\phi_*(\theta_*(t)) = \theta'_*(\phi_*(t)).

Proposition 9

Let G1,…,GnG_1, \ldots, G_n be Lie groups and G=G1×⋯×GnG = G_1 \times \cdots \times G_n. If the vector spaces T(∞)(G)\mathscr{T}^{(\infty)}(G) and T(∞)(G1)⊗⋯⊗T(∞)(Gn)\mathscr{T}^{(\infty)}(G_1) \otimes \cdots \otimes \mathscr{T}^{(\infty)}(G_n) are canonically identified, the algebra T(∞)(G)\mathscr{T}^{(\infty)}(G) is the tensor product of the algebras T(∞)(G1),…,T(∞)(Gn)\mathscr{T}^{(\infty)}(G_1), \ldots, \mathscr{T}^{(\infty)}(G_n). If ti∈T(∞)(Gi)t_i \in \mathscr{T}^{(\infty)}(G_i) for i=1,…,ni = 1, \ldots, n, then

(t1⊗⋯⊗tn)∨=t1∨⊗⋯⊗tn∨. (t_1 \otimes \cdots \otimes t_n)^\vee = t_1^\vee \otimes \cdots \otimes t_n^\vee.

It suffices to consider the case n=2n = 2. Let t1,t1′t_1, t_1' be in T(∞)(G1)\mathscr{T}^{(\infty)}(G_1), t2,t2′t_2, t_2' in T(∞)(G2)\mathscr{T}^{(\infty)}(G_2). We need to show that (t1⊗t2)∗(t1′⊗t2′)=(t1∗t1′)⊗(t2∗t2′)(t_1 \otimes t_2) * (t_1' \otimes t_2') = (t_1 * t_1') \otimes (t_2 * t_2') and that (t1⊗t2)∨=t1∨⊗t2∨(t_1 \otimes t_2)^\vee = t_1^\vee \otimes t_2^\vee. Consider the diagram

G×G→sG×G↓n↓mGG \begin{array}{ccc} G \times G & \xrightarrow{s} & G \times G \\ \downarrow n & & \downarrow m \\ G & & G \end{array}

where m((x1,x2),(x1′,x2′))=(x1x1′,x2x2′)m((x_1, x_2), (x_1', x_2')) = (x_1 x_1', x_2 x_2'),

n((x1,x2),(x1′,x2′))=((x1,x1′),(x2,x2′)), n((x_1, x_2), (x_1', x_2')) = ((x_1, x_1'), (x_2, x_2')),

p1(x1,x1′)=x1x1′p_1(x_1, x_1') = x_1 x_1', p2(x2,x2′)=x2x2′p_2(x_2, x_2') = x_2 x_2'. This diagram is commutative. Hence

m∗((t1⊗t2)⊗(t1′⊗t2′))=(p1⊗p2)∗(n∗((t1⊗t2)⊗(t1′⊗t2′))), m_*((t_1 \otimes t_2) \otimes (t_1' \otimes t_2')) = (p_1 \otimes p_2)_*(n_*((t_1 \otimes t_2) \otimes (t_1' \otimes t_2'))),

that is

(t1⊗t2)∗(t1′⊗t2′)=(p1⊗p2)∗((t1⊗t1′)⊗(t2⊗t2′))=p1∗(t1⊗t1′)⊗p2∗(t2⊗t2′)=(t1∗t1′)⊗(t2∗t2′). \begin{align*} (t_1 \otimes t_2) * (t_1' \otimes t_2') &= (p_1 \otimes p_2)_*((t_1 \otimes t_1') \otimes (t_2 \otimes t_2')) \\ &= p_1*(t_1 \otimes t_1') \otimes p_2*(t_2 \otimes t_2') \\ &= (t_1 * t_1') \otimes (t_2 * t_2'). \end{align*}

It is seen analogously that (t1⊗t2)∨=t1∨⊗t2∨(t_1 \otimes t_2)^\vee = t_1^\vee \otimes t_2^\vee.

Proposition 10

Let H be a Lie subgroup of G and i:H→Gi : H \to G the canonical injection. Then i∗i_* is an injective homomorphism of the algebra T(∞)(H)\mathscr{T}^{(\infty)}(H) into the algebra T(∞)(H)\mathscr{T}^{(\infty)}(H) and i∗(t∨)=(i∗(t))∨i_*(t^\vee) = (i_*(t))^\vee for all t∈T(∞)(H)t \in \mathscr{T}^{(\infty)}(H).

This follows from Propositions 6 and 8 and Differentiable and Analytic Manifolds, R, 13.2.3.

T(∞)(H)\mathscr{T}^{(\infty)}(H) is identified with a subalgebra of T(∞)(G)\mathscr{T}^{(\infty)}(G) by means of the isomorphism of Proposition 10.

Remark

Proposition 10 remains valid if H is a Lie quasi-subgroup.

We recall (Differentiable and Analytic Manifolds, R, 13.5.1) that, if V is an analytic manifold over K, T(∞)(V)\mathscr{T}^{(\infty)}(V) has canonically a cogebra structure over K with a counit; the counit is the linear mapping of T(∞)(G)\mathscr{T}^{(\infty)}(G) into K which associates with each element of Tx(∞)(V)T_x^{(\infty)}(V) its constant term.

Proposition 11

Let G be a Lie group. (i) The cogebra T(∞)(G)\mathscr{T}^{(\infty)}(G), with convolution, is a bigebra (Algebra, Chapter III, § 11, no. 4). (ii) Let c be the coproduct on T(∞)(G)\mathscr{T}^{(\infty)}(G). Let t∈T(∞)(G)t \in \mathscr{T}^{(\infty)}(G) and write

c(t)=∑i=1nti⊗ti′. c(t) = \sum_{i=1}^n t_i \otimes t_i'.
Then c(t∨)=∑i=1nti∨⊗ti′∨c(t^\vee) = \sum_{i=1}^n t_i^\vee \otimes t_{i'}^\vee.

We prove (i). In the definition of bigebra referred to, condition (1) follows from Propositions 2 and 3 and condition (2) follows from Differentiable and Analytic Manifolds, R, 13.5.1. Let d be the mapping g↦(g,g)g \mapsto (g, g) of G into G×GG \times G. Then c=d∗c = d_* and hence c is an algebra morphism (Propositions 6 and 9), which is condition (3). Let t∈Tg(∞)(G)t \in T_g^{(\infty)}(G), t′∈Tg′(∞)(G)t' \in T_{g'}^{(\infty)}(G) have no constant term and λ,λ′\lambda, \lambda' be elements of K; then εg⊗t′,t⊗εg′,t⊗t′\varepsilon_g \otimes t', t \otimes \varepsilon_{g'}, t \otimes t' are without constant term (Differentiable and Analytic Manifolds, R, 13.4.1) and hence the constant term of (λεg+t)∗(λ′εg′+t′)(\lambda \varepsilon_g + t) * (\lambda' \varepsilon_{g'} + t') is λλ′\lambda \lambda'; hence condition (4) holds.

We prove (ii). By Propositions 8 and 9,

c(t∨)=d∗(t∨)=(d∗(t))∨=(∑i=1nti⊗ti′)∨=∑i=1nti′∨⊗ti′∨. c(t^\vee) = d_*(t^\vee) = (d_*(t))^\vee = \left( \sum_{i=1}^n t_i \otimes t_i' \right)^\vee = \sum_{i=1}^n t_{i'}^\vee \otimes t_{i'}^\vee.

Proposition 12

Let G, H be two Lie groups and ϕ\phi a morphism of G into H. Then ϕ∗\phi_* is a bigebra morphism of T(∞)(G)\mathscr{T}^{(\infty)}(G) into T(∞)(H)\mathscr{T}^{(\infty)}(H).

This follows from Proposition 6 and Differentiable and Analytic Manifolds, R, 13.5.1.

Let G be a Lie group. The restrictions of the convolution and the coproduct to U(G) define a bigebra structure on U(G). We have U(G)^{\vee} = U(G). If ϕ:G→H\phi : G \to H is a Lie group morphism, we denote by U(ϕ\phi) the mapping t↦ϕ∗(t)t \mapsto \phi_*(t) of U(G) into U(H); this is a bigebra morphism. If ψ:H→L\psi : H \to L is another Lie group morphism, then U(ψ∘ϕ\psi \circ \phi) = U(ψ\psi) \circ U(ϕ\phi). If ϕ\phi is an immersion (resp. a submersion), U(ϕ\phi) is injective (resp. surjective) by Differentiable and Analytic Manifolds, R, 13.2.3. In particular, if H is a Lie subgroup of G, U(H) is identified with a subalgebra of U(G), the coproduct on U(H) being the restriction of the coproduct on U(G). If H is open in G, then U(H) = U(G). If G_1, G_2 are Lie groups, U(G_1 \times G_2) is identified with U(G_1) \times U(G_2). The primitive elements of U(G) are those of T_e(G) (Differentiable and Analytic Manifolds, R, 13.5.3).

Again let ϕ:G→H\phi : G \to H be a Lie group morphism. If gr U(G) is identified TS(T_e(G)) and gr U(H) with TS(T_e(H)), then gr U(ϕ\phi) is identified with TS(T_e(ϕ\phi)) (Differentiable and Analytic Manifolds, R, 13.3.5). We apply this to the isomorphism g↦g−1g \mapsto g^{-1} of G onto G^{\vee}; then T_e(ϕ\phi) = -1 and hence

t∈Us(G)⇒t∨≡(−1)stmod  Us−1(G). t \in U_s(G) \Rightarrow t^{\vee} \equiv (-1)^s t \mod U_{s-1}(G).

3. Case of a group operating on a manifold

Let G be a Lie group, X a manifold of class C^r and f a law of left operation of class C^r of G on X. If t∈Tg(s)(G)t \in T^{(s)}_g(G) and u∈Tx(s′)(X)u \in T^{(s')}_x(X) and s+s′≤rs + s' \leq r, we denote by t∗ut * u the image of t⊗ut \otimes u under f∗f_*. We extend the product \* to a bilinear mapping also denoted by *, of T(s)(G)+T(s′)(X)\mathscr{T}^{(s)}(G) + \mathscr{T}^{(s')}(X) into T(s+s′)(X)\mathscr{T}^{(s+s')}(X). Proposition 1 of no. 1 can be extended with obvious modifications to the present situation.

When G operates on itself by left translation, we recover Definition 1 of no. 1.

Proposition 13

Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G), t′∈T(s′)(G)t' \in \mathscr{T}^{(s')}(G), u∈T(s′′)(X)u \in \mathscr{T}^{(s'')}(X), such that

s+s′+s′′≤r. s + s' + s'' \leq r.

Then (t∗t′)∗u=t∗(t′∗u)(t * t') * u = t * (t' * u).

This can be proved as is Proposition 2 of no. 1.

In particular, if r≤∞r \leq \infty, the vector space T(∞)(X)\mathscr{T}^{(\infty)}(X) is a left module over the algebra T(∞)(G)\mathscr{T}^{(\infty)}(G) with the product *.

Proposition 14

(i) Let g0∈Gg_0 \in G and τ(g0)\tau(g_0) be the mapping x↦f(g0,x)x \mapsto f(g_0, x) of X into X. If u∈T(r)(X)u \in \mathscr{T}^{(r)}(X), then τ(g0)∗u=εg0∗u\tau(g_0)*u = \varepsilon_{g_0}*u.

(ii) Let x0∈Xx_0 \in X and ϱ(x0)\varrho(x_0) be the mapping g↦f(g,x0)g \mapsto f(g, x_0) of G into X. If t∈T(r)(G)t \in T^{(r)}(G), then ϱ(x0)∗t=t∗εx0\varrho(x_0)*t = t*\varepsilon_{x_0}.

This can be proved as is Proposition 3 of no. 1.

In particular, if u∈T(X)u \in T(X) and t∈T(G)t \in T(G), εg0∗u\varepsilon_{g_0} * u and t∗εx0t * \varepsilon_{x_0} are equal to the products g0ug_0u and tx0tx_0 defined in § 2, no. 2.

Proposition 15

Let G (resp. G') be a Lie group and X (resp. X') a manifold of class C^r. Suppose that a law of left operation of class C^r of G (resp. G') on X (resp. X') is given. Let ϕ\phi be a morphism of G into G' and ψ\psi a ϕ\phi-morphism of X into X'. Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G), u∈T(s′)(X)u \in T^{(s')}(X) be such that s+s′≤rs + s' \leq r. Then

ψ∗(t∗u)=ϕ∗(t)∗ψ∗(u). \psi_*(t * u) = \phi_*(t) * \psi_*(u).
This can be proved as is Proposition 6 of no. 2.

Remark

Let f be a law of right operation of class C^r of G on X. If t∈T(s)(G)t \in \mathscr{T}^{(s)}(G) and u∈T(s′)(X)u \in \mathscr{T}^{(s')}(X), with s+s′≤rs + s' \leq r, we denote by u∗tu * t the image of u⊗tu \otimes t under f∗f_*. Propositions 13, 14, 15 go over to this situation in an obvious way.

Proposition 16

Let G, G' be Lie groups, X a manifold of class C^r and suppose that G (resp. G') operates on X on the left (resp. right), with (gx)g′=g(xg′)(gx)g' = g(xg') for all x∈X,g∈G,g′∈G′x \in X, g \in G, g' \in G'. Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G), t′∈T(s′)(G′)t' \in \mathscr{T}^{(s')}(G'), t′′∈T(s′′)(X)t'' \in T^{(s'')}(X), with s+s′+s′′≤rs + s' + s'' \leq r. Then

(t∗t′′)∗t′=t∗(t′′∗t′). (t * t'') * t' = t * (t'' * t').
(t∗t′′)∗t′(t * t'') * t' (resp. t∗(t′′∗t′)t * (t'' * t')) is the image of t⊗t′′⊗t′t \otimes t'' \otimes t' under the mapping (g,x,g′)↦(gx)g′(g, x, g') \mapsto (gx)g' (resp. g(xg′)g(xg')) of G×X×G′G \times X \times G' into X.

4. Convolution of point distributions and functions

Let G be a Lie group, X a manifold of class C^r and (g,x)↦gx(g, x) \mapsto gx a law of left operation of class C^r of G on X. For all x∈Xx \in X, let ϱ(x)\varrho(x) denote the orbital mapping of x.

Definition 3

Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G) with s≤rs \leq r. Let f:X→Ff : X \to F be a function of class C^r with values in a Hausdorff polynormed space (for example F=KF = \mathbf{K}). The convolution of t and f, denoted by t∗ft * f, is the function on X with values in F defined by

(t∗f)(x)=⟨t∨∗εx,f⟩. (t * f)(x) = \langle t^\vee * \varepsilon_x, f \rangle.
Then
(t∗f)(x)=⟨ϱ(x)∗(t∨),f⟩(no. 3, Proposition 14 (ii))=⟨t∨,f∘ϱ(x)⟩(Diff. & Anal. Man., R, 13.2.3)=⟨t,(f∘ϱ(x))∨⟩(Diff. & Anal. Man., R, 13.2.3). \begin{align*} (t * f)(x) &= \langle \varrho(x)_*(t^\vee), f \rangle \quad \text{(no. 3, Proposition 14 (ii))} \\ &= \langle t^\vee, f \circ \varrho(x) \rangle \quad \text{(Diff. \& Anal. Man., R, 13.2.3)} \\ &= \langle t, (f \circ \varrho(x))^\vee \rangle \quad \text{(Diff. \& Anal. Man., R, 13.2.3)}. \end{align*}
Note that Definition 3 can also be written in the more symmetric form
⟨εx,t∗f⟩=⟨t∨∗εx,f⟩. \langle \varepsilon_x, t * f \rangle = \langle t^\vee * \varepsilon_x, f \rangle.
The function (g,x)↦f(gx)=(f∘ϱ(x))(g)(g, x) \mapsto f(gx) = (f \circ \varrho(x))(g) on G×XG \times X is of class C^r. By Differentiable and Analytic Manifolds, R, 13.4.4, the function x↦⟨t∨,f∘ϱ(x)⟩x \mapsto \langle t^\vee, f \circ \varrho(x) \rangle is therefore of class Cr−sC^{r-s} if s<∞s < \infty. In other words, if s<∞s < \infty, t∗ft * f is of class Cr−sC^{r-s}.

Clearly t∗ft * f depends linearly on tt and ff.

Formula (4) implies in particular, for g∈Gg \in G,

(εg∗f)(x)=f(g−1x) (\varepsilon_g * f)(x) = f(g^{-1}x)
that is
εg∗f=γ(g)f. \varepsilon_g * f = \gamma(g)f.

Suppose that K=RK = \mathbf{R} or C\mathbf{C}, that GG and XX are finite-dimensional and that XX has a positive measure invariant under GG. The definition of εg∗f\varepsilon_g * f agrees with that of Integration, Chapter VIII, § 4, no. 1 (cf. formula (2), loc. cit.).

Proposition 17

Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G), t′∈T(s′)(X)t' \in \mathscr{T}^{(s')}(X) and f:X→Ff : X \to F a function of class CrC^r with s+s′≤rs + s' \leq r. Then

⟨t′,t∗f⟩=⟨t∨∗t′,f⟩. \langle t', t * f \rangle = \langle t^\vee * t', f \rangle.
⟨t′,t∗f⟩=⟨t′,x↦⟨t,g↦f(g−1x)⟩⟩by (4)=⟨t⊗t′,(g,x)↦f(g−1x)⟩(Diff. & Anal. Man., R, 13.4.4)=⟨t∨⊗t′,(g,x)↦f(gx)⟩(Diff. & Anal. Man., R, 13.2.3)=⟨t∨∗t′,f⟩. \begin{align*} \langle t', t * f \rangle &= \langle t', x \mapsto \langle t, g \mapsto f(g^{-1}x) \rangle \rangle \quad \text{by (4)} \\ &= \langle t \otimes t', (g, x) \mapsto f(g^{-1}x) \rangle \quad (\text{Diff. \& Anal. Man., R, 13.4.4}) \\ &= \langle t^\vee \otimes t', (g, x) \mapsto f(gx) \rangle \quad (\text{Diff. \& Anal. Man., R, 13.2.3}) \\ &= \langle t^\vee * t', f \rangle. \end{align*}

Proposition 18

Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G), t′∈T(s′)(G)t' \in \mathscr{T}^{(s')}(G) and f:X→Ff : X \to F a function of class CrC^r, with s+s′≤rs + s' \leq r. Then

(t∗t′)∗f=t∗(t′∗f). (t * t') * f = t * (t' * f).
For all x∈Xx \in X,
⟨εx,(t∗t′)∗f⟩=⟨((t∗t′)∨∗εx),f⟩by (5)=⟨t′∨∗(t∨∗εx),f⟩(Propositions 2 and 7)=⟨t∨∗εx,t′∗f⟩(Proposition 17)=⟨εx,t∗(t′∗f)⟩(Proposition 17). \begin{align*} \langle \varepsilon_x, (t * t') * f \rangle &= \langle ((t * t')^\vee * \varepsilon_x), f \rangle \quad \text{by (5)} \\ &= \langle {t'}^\vee * (t^\vee * \varepsilon_x), f \rangle \quad (\text{Propositions 2 and 7}) \\ &= \langle t^\vee * \varepsilon_x, t' * f \rangle \quad (\text{Proposition 17}) \\ &= \langle \varepsilon_x, t * (t' * f) \rangle \quad (\text{Proposition 17}). \end{align*}

If r≥∞r \geq \infty, we see that the set of functions of class C∞C^\infty on XX with values in FF is a left module over the algebra T(∞)(G)\mathscr{T}^{(\infty)}(G).

Proposition 19

Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G), with s≤rs \leq r. Let ff (resp. f′f') be a function of class CrC^r on XX with values in a Hausdorff polynormed space FF (resp. F′F'). Let (u,u′)↦uu′(u, u') \mapsto uu' be a continuous bilinear mapping of F×F′F \times F' into a Hausdorff polynormed space F′′F'', so that ff′ff' is a function of class CrC^r on XX with values in F′′F''. Let

∑i=1nti⊗ti′ be the image of t in T(s)(G)⊗T(s)(G) under the coproduct. Then \sum_{i=1}^n t_i \otimes t'_i \text{ be the image of } t \text{ in } \mathscr{T}^{(s)}(G) \otimes \mathscr{T}^{(s)}(G) \text{ under the coproduct. Then}
t∗(ff′)=∑i=1n(ti∗f)(ti′∗f′). t * (ff') = \sum_{i=1}^n (t_i * f)(t'_i * f').

Let x∈Xx \in X and let ρ(x)\rho(x) denote the orbital mapping of xx. Then

⟨εx,t∗(ff′)⟩=⟨t∨,(ff′)∘ρ(x)⟩by (4)=⟨t∨,(f∘ρ(x))(f′∘ρ(x))⟩=∑i=1n⟨ti∨,f∘ρ(x)⟩⟨ti′∨,f′∘ρ(x)⟩=∑i=1n⟨εx,ti∗f⟩⟨εx,ti′∗f′⟩by (4).(Diff. & Man. Anal., R, 13.5.2) \langle \varepsilon_x, t * (ff') \rangle = \langle t^\vee, (ff') \circ \rho(x) \rangle \quad \text{by (4)} \\ = \langle t^\vee, (f \circ \rho(x))(f' \circ \rho(x)) \rangle \\ = \sum_{i=1}^n \langle t_i^\vee, f \circ \rho(x) \rangle \langle t_{i'}^\vee, f' \circ \rho(x) \rangle \tag{Diff. \& Man. Anal., R, 13.5.2} \\ = \sum_{i=1}^n \langle \varepsilon_x, t_i * f \rangle \langle \varepsilon_x, t_i' * f' \rangle \quad \text{by (4).}

Remark 1

Let G be a Lie group, X a manifold of class CrC^r and (x,g)↦xg(x, g) \mapsto xg a law of right operation of class CrC^r of G on X. If t∈T(s)(G)t \in \mathscr{T}^{(s)}(G) with s≤rs \leq r and f:X→Ff : X \to F is a function of class CrC^r on X, we denote by f∗tf * t the function on X defined by

⟨εx,f∗t⟩=⟨εx∗t∨,f⟩=⟨ρ(x)∗(t∨),f⟩=⟨t∨,f∘ρ(x)⟩=⟨t,(f∘ρ(x))∨⟩. \langle \varepsilon_x, f * t \rangle = \langle \varepsilon_x * t^\vee, f \rangle \\ = \langle \rho(x) * (t^\vee), f \rangle \\ = \langle t^\vee, f \circ \rho(x) \rangle \\ = \langle t, (f \circ \rho(x))^\vee \rangle.
In particular
(f∗εg)(x)=f(xg−1) (f * \varepsilon_g)(x) = f(xg^{-1})
that is
f∗εg=δ(g)−1f. f * \varepsilon_g = \delta(g)^{-1} f.
Propositions 17, 18, 19 become, in the obvious notation,
⟨t′,f∗t⟩=⟨t′∗t∨,f⟩(11) \langle t', f * t \rangle = \langle t' * t^\vee, f \rangle \tag{11}
f∗(t∗t′)=(f∗t)∗t′(12) f * (t * t') = (f * t) * t' \tag{12}
(ff′)∗t=∑i=1n(f∗ti)(f′∗ti′)(13) (ff') * t = \sum_{i=1}^n (f * t_i)(f' * t_i') \tag{13}

Proposition 20

Let G, G' be Lie groups, X a manifold of class CrC^r and (g,x)↦gx(g, x) \mapsto gx (resp. (x,g′)↦xg′(x, g') \mapsto xg') a law of left (resp. right) operation of class CrC^r of G (resp. G') on X. Suppose that (gx)g′=g(xg′)(gx)g' = g(xg') for all x∈X,g∈G,g′∈G′x \in X, g \in G, g' \in G'. Let t∈T(s)(G)t \in \mathscr{T}^{(s)}(G), t′∈T(s′)(G′)t' \in \mathscr{T}^{(s')}(G') and f:X→Ff : X \to F be a function of class CrC^r such that s+s′≤rs + s' \leq r. Then*

(t∗f)∗t′=t∗(f∗t′). (t * f) * t' = t * (f * t').
For all x∈Xx \in X,
⟨εx,(t∗f)∗t′⟩=⟨εx∗t′∨,t∗f⟩by (8)=⟨t∨∗(εx∗t′∨),f⟩(Proposition 17)=⟨t∨∗εx,f∗t′⟩(Proposition 2 and (11))=⟨εx,t∗(f∗t′)⟩by (5). \langle \varepsilon_x, (t * f) * t' \rangle = \langle \varepsilon_x * {t'}^\vee, t * f \rangle \quad \text{by (8)} \\ = \langle t^\vee * (\varepsilon_x * {t'}^\vee), f \rangle \quad \text{(Proposition 17)} \\ = \langle t^\vee * \varepsilon_x, f * t' \rangle \quad \text{(Proposition 2 and (11))} \\ = \langle \varepsilon_x, t * (f * t') \rangle \quad \text{by (5).}

In particular, consider G as operating on itself by left and right translations. If f:G→Ff : G \to F is a function of class CrC^r on G and t∈T(s)(G)t \in \mathscr{T}^{(s)}(G) (with s≤rs \leq r), t∗ft * f and f∗tf * t are, if s<∞s < \infty, functions of class Cr−sC^{r-s} on G. Further, let t′∈T(s′)(G)t' \in \mathscr{T}^{(s')}(G), with s+s′≤rs + s' \leq r. Then

(t∗f)∗t′=t∗(f∗t′). (t * f) * t' = t * (f * t').
In particular, C∞(G)\mathscr{C}^\infty(G) is a (T(∞)(G),T(∞)(G))(\mathscr{T}^{(\infty)}(G), \mathscr{T}^{(\infty)}(G))-bimodule. Formulae (5) and (8) admit as special cases
⟨t,f⟩=⟨εe,t∨∗f⟩=⟨εe,f∗t∨⟩. \langle t, f \rangle = \langle \varepsilon_e, t^\vee * f \rangle = \langle \varepsilon_e, f * t^\vee \rangle.

Remark 2

Let (g,x)↦gx(g, x) \mapsto gx be a law of left operation of class CrC^r of G on X. Let t∈Us(G)t \in U_s(G) with s≤rs \leq r, Ω\Omega be an open subset of X and f:Ω→Ff : \Omega \to F a function of class CrC^r. t∗ft * f can also be defined by formula (4) or (5); it is a function defined on Ω\Omega with values in F, of class Cr−sC^{r-s} if s<∞s < \infty. The results of this no. extend in an obvious way to this situation.

5. Fields of point distributions defined by the action of a group on a manifold

Let (g,x)↦λ(g,x)=gx(g, x) \mapsto \lambda(g, x) = gx be a law of left operation of class CrC^r of G on X. Let s≤rs \leq r and t∈Us(G)t \in U_s(G). For all x∈Xx \in X, t∗εx∈Tx(s)(X)t * \varepsilon_x \in T^{(s)}_x(X). The mapping x↦t∗εxx \mapsto t * \varepsilon_x is called the field of point distributions defined by t and the action of G on X and denoted sometimes by DtλD_t^\lambda or simply DtD_t. Let Ω\Omega be an open subset of X and F a Hausdorff polynormed space. If f:Ω→Ff : \Omega \to F is of class CrC^r and s≤rs \leq r, the function t∨∗ft^\vee * f on Ω\Omega is also denoted by DtfD_t f. Then

(Dtf)(x)=⟨t∗εx,f⟩. (D_t f)(x) = \langle t * \varepsilon_x, f \rangle.
If s<∞s < \infty, then Dtf∈Cr−s(Ω,F)D_t f \in \mathscr{C}^{r-s}(\Omega, F) by no. 4. Thus f↦Dtff \mapsto D_t f is a mapping of Cr(Ω,F)\mathscr{C}^r(\Omega, F) into Cr−s(Ω,F)\mathscr{C}^{r-s}(\Omega, F) (often denoted by DtD_t by an abuse of notation). If t∈Us(G)t \in U_s(G), t′∈Us′(G)t' \in U_{s'}(G) and s+s′≤rs + s' \leq r, then, by Proposition 18 of no. 4,
Dt∗t′=Dt′(Dtf) D_{t*t'} = D_{t'}(D_t f)
and hence, using the abuse of notation indicated above,
Dt∗t′=Dt′∘Dt. D_{t*t'} = D_{t'} \circ D_t.
Suppose that G and X are finite-dimensional. The mapping (t,x)↦t⊗εx(t, x) \mapsto t \otimes \varepsilon_x of T(s)(G)×XT^{(s)}(G) \times X into the vector bundle T(s)(G×X)T^{(s)}(G \times X) (cf. Differentiable and Analytic Manifolds, R, 13.2.5) is of class Cr−sC^{r-s}. Hence (Differentiable and Analytic Manifolds, R, 13.2.5) the mapping (t,x)↦t∗εx(t, x) \mapsto t * \varepsilon_x of T(s)(G)×XT^{(s)}(G) \times X into the vector bundle T(s)(X)T^{(s)}(X) is of class Cr−sC^{r-s}. In particular, DtD_t is a differential operator of order ≤s\leq s and class Cr−sC^{r-s} in the sense of Differentiable and Analytic Manifolds, R, 14.1.6. By formula (16), the function DtfD_t f is then the image of ff under this differential operator (Differentiable and Analytic Manifolds, R, 14.1.4).

We now no longer suppose that G and X are finite-dimensional. Let ψ\psi be an automorphism of the manifold X and Δ\Delta a field of point distributions on X. Conforming with the general definitions, the transform of Δ\Delta under ψ\psi is the field of point distributions on X whose value at ψ(x)\psi(x) is ψ∗(Δ(x))\psi_*(\Delta(x)); we denote this mapping by ψ(Δ)\psi(\Delta). If g∈Gg \in G and τ(g)\tau(g) denotes the automorphism x↦gxx \mapsto gx of X, the transform of Δ\Delta under τ(g)\tau(g) is also called the transform of Δ\Delta under g.

Proposition 21

Let ψ\psi be an automorphism of X commuting with the operations of G. Then DtD_t is invariant under ψ\psi.

For all x∈Xx \in X,

(ψ(Dt))(ψ(x))=ψ∗(Dt(x))=ψ∗(t∗εx)=t∗ψ∗(εx)=t∗εψ(x)=Dt(ψ(x)). \begin{align*} (\psi(D_t))(\psi(x)) &= \psi_*(D_t(x)) = \psi_*(t * \varepsilon_x) \\ &= t * \psi_*(\varepsilon_x) \tag{Proposition 15} \\ &= t * \varepsilon_{\psi(x)} = D_t(\psi(x)). \end{align*}

Proposition 22

If g∈Gg \in G, the transform of DtD_t under g is Dεg∗t∗εg−1D_{\varepsilon_g * t * \varepsilon_g^{-1}}.

The value of this transform at gxgx is

τ(g)∗(Dt(x))=τ(g)∗(t∗εx)=εg∗(t∗εx)(Proposition 14 (i))=(εg∗t∗εg−1)∗εgx(Propositions 1 and 2)=Dεg∗t∗εg−1(gx). \begin{align*} \tau(g)_*(D_t(x)) &= \tau(g)_*(t * \varepsilon_x) \\ &= \varepsilon_g * (t * \varepsilon_x) \quad \text{(Proposition 14 (i))} \\ &= (\varepsilon_g * t * \varepsilon_g^{-1}) * \varepsilon_{gx} \quad \text{(Propositions 1 and 2)} \\ &= D_{\varepsilon_g * t * \varepsilon_g^{-1}}(gx). \end{align*}

Let (x,g)↦μ(x,g)=xg(x, g) \mapsto \mu(x, g) = xg be a law of right operation of class C′C' of G on X. Let s≤rs \leq r and t∈Us(G)t \in U_s(G). For all x∈Xx \in X, εx∗t∈Tx(s)(X)\varepsilon_x * t \in T^{(s)}_x(X). The mapping x↦εx∗tx \mapsto \varepsilon_x * t is called the field of distributions defined by t and the action of G on X and is sometimes denoted by DtuD_t^u or simply DtD_t. Let Ω\Omega be an open subset of X. If f:Ω→Ff : \Omega \to F is of class C′C', the function f∗t∨f * t^\vee is denoted by DtfD_t f. Then

(19)(19)
(Dtf)(x)=⟨εx∗t,f⟩(D_t f)(x) = \langle \varepsilon_x * t, f \rangle

and, in the obvious notation,

(20)(20)
Dt∗t′f=Dt(Dt′f)D_{t * t'} f = D_t(D_{t'} f)
(21)(21)
Dt∗t′=Dt∘Dt′.D_{t * t'} = D_t \circ D_{t'}.

Proposition 21 remains valid. Let g∈Gg \in G. The transform of DtD_t under g (that is under the automorphism x↦xgx \mapsto xg of X) is Dεg−1∗t∗εgD_{\varepsilon_g^{-1} * t * \varepsilon_g}.

6. Invariant fields of point distributions on a Lie group

Definition 4

Let G be a Lie group. A field of distributions on G is called left (resp. right) invariant if it is invariant under left (resp. right) translations of G.

In other words, a field of distributions g↦Δgg \mapsto \Delta_g on GG is left invariant if

Δgg′=γ(g)∗βg′ \Delta_{gg'} = \gamma(g) * \beta_{g'}
for g,g′g, g' in GG, or again if
Δgg′=εg∗Δg′ \Delta_{gg'} = \varepsilon_g * \Delta_{g'}
for g,g′g, g' in GG. It is right invariant if
Δgg′=δ(g′−1)∗Δg \Delta_{gg'} = \delta({g'}^{-1}) * \Delta_g
for g,g′g, g' in GG, or again if:
Δgg′=Δg∗εg, \Delta_{gg'} = \Delta_g * \varepsilon_g,
for g,g′g, g' in GG.

Definition 5

Let GG be a Lie group and t∈U(G)t \in U(G). Let LtL_t denote the field of distributions g↦εg∗tg \mapsto \varepsilon_g * t on GG and RtR_t the field of distributions g↦t∗εgg \mapsto t * \varepsilon_g on GG.

In other words, LtL_t (resp. RtR_t) is the field of distributions defined by tt and GG operating on GG on the right (resp. left) by means of the mapping (g,g′)↦gg′(g, g') \mapsto gg'. Let Ω\Omega be an open subset of GG and FF a Hausdorff polynormed space; if f∈Cω(Ω,F)f \in C^\omega(\Omega, F), then Ltf=f∗t∨∈Cω(Ω,F)L_t f = f * t^\vee \in C^\omega(\Omega, F) and

Rtf=t∨∗f∈Cω(Ω,F) R_t f = t^\vee * f \in C^\omega(\Omega, F)
(no. 5). If GG is finite-dimensional, the differential operators LtL_t and RtR_t are of class CωC^\omega (no. 5).

Proposition 23

(i) The mapping t↦Ltt \mapsto L_t (resp. t↦Rtt \mapsto R_t) is an isomorphism of the vector space U(G)U(G) onto the vector field of left (resp. right) invariant distributions on GG. (ii) For t,t′t, t' in U(G)U(G), Lt∗t′=Lt∘Lt′L_{t*t'} = L_t \circ L_{t'}, Rt∗t′=Rt′∘RtR_{t*t'} = R_{t'} \circ R_t, Lt∘Rt′=Rt′∘LtL_t \circ R_{t'} = R_{t'} \circ L_t (with the abuse of notation of no. 5). (iii) If θ\theta is the mapping g↦g−1g \mapsto g^{-1} of GG onto GG, then θ(Lt)=Rt∨\theta(L_t) = R_{t^\vee}. (iv) *If t∈U(G)t \in U(G) and g∈Gg \in G, then (Lt)g=(Rεg∗t∗εg−1)g(L_t)_g = (R_{\varepsilon_g * t * \varepsilon_g^{-1}})_g.

In GG every right translation commutes with every left translation. By Proposition 21 of no. 5, LtL_t is therefore left invariant. As (Lt)e=t(L_t)_e = t, the mapping t↦Ltt \mapsto L_t is injective. Let Δ\Delta be a field of left invariant distributions on GG; let t=Δet = \Delta_e; then Δ\Delta and LtL_t have the same value at ee and are left invariant and hence Δ=Lt\Delta = L_t. This proves (i) for LtL_t and the argument is similar for RtR_t. The formulae Lt∗t′=Lt∘Lt′L_{t*t'} = L_t \circ L_{t'}, Rt∗t′=Rt′∘RtR_{t*t'} = R_{t'} \circ R_t follow from (21) and (18). Let t∈Us(G)t \in U_s(G), t′∈Us′(G)t' \in U_{s'}(G), f∈Cr(Ω,F)f \in C^r(\Omega, F), where Ω\Omega is open in GG and s+s′≤rs + s' \leq r; then

LtRt′f=Lt(t′∨∗f)=(t′∨∗f)∗t=t′∨∗(f∗t∨)=Rt′Ltf \begin{align*} L_t R_{t'} f &= L_t ({t'}^\vee * f) = ({t'}^\vee * f) * t \\ &= {t'}^\vee * (f * t^\vee) \tag{Proposition 20} \\ &= R_{t'} L_t f \end{align*}
and hence Lt∘Rt′=Rt′∘LtL_t \circ R_{t'} = R_{t'} \circ L_t. As θ\theta is an isomorphism of GG onto G∨G^\vee, θ(Lt)\theta(L_t) is a field of right invariant distributions on GG; its value at ee is θ(t)=t∨\theta(t) = t^\vee; hence θ(Lt)=Rt∨\theta(L_t) = R_{t^\vee}. Finally,
(Lt)g=εg∗t=(εg∗t∗εg−1)∗εg=(Rεg∗t∗εg−1)g. (L_t)_g = \varepsilon_g * t = (\varepsilon_g * t * \varepsilon_g^{-1}) * \varepsilon_g = (R_{\varepsilon_g * t * \varepsilon_g^{-1}})_g.

Remark 1

It is the action of G on itself by right translation which defines the fields of left invariant distributions.

Remark 2

Suppose that G is finite-dimensional. The mapping

(t,g)↦(Rt)g=t∗εg(t, g) \mapsto (\mathbf{R}_t)_g = t * \varepsilon_g

of Us(G)×GU_s(G) \times G into T(s)(G)T^{(s)}(G) is an isomorphism of analytic vector bundles; for this mapping is bijective, linear on each fibre and analytic (no. 5); on the other hand, let ϕ:T(s)(G)→Us(G)×G\phi : T^{(s)}(G) \to U_s(G) \times G be the inverse bijection; if t∈Tg(s)(G)t \in T^{(s)}_g(G), then ϕ(t)=(t∗εg−1,g)\phi(t) = (t * \varepsilon_{g^{-1}}, g) and hence ϕ\phi is analytic. The isomorphism ϕ\phi is called the right trivialization of T(s)(G)T^{(s)}(G). Similarly, consider the mapping (t,g)↦(Lt)g=εg∗t(t, g) \mapsto (\mathbf{L}_t)_g = \varepsilon_g * t of Ug(G)×GU_g(G) \times G into T(s)(G)T^{(s)}(G); the inverse isomorphism is called the left trivialization of T(s)(G)T^{(s)}(G). By restriction we recover the right and left trivializations of T(G)T(G) (§ 2, no. 2).

7. Lie algebra of a Lie group

Let G be a Lie group. In U(G)U(G), as in any associative algebra, we write [t,t′]=t∗t′−t′∗t[t, t'] = t * t' - t' * t. As Te(G)T_e(G) is the set of primitive elements of U(G)U(G), [Te(G),Te(G)]⊂Te(G)[T_e(G), T_e(G)] \subset T_e(G) (Chapter II, § 1, no. 2, Proposition 4). The restriction of the bracket to Te(G)T_e(G) therefore defines on Te(G)T_e(G) a Lie algebra structure.

Lemma 1

Let X and X′X' be complete normable spaces, X0X_0 an open neighbourhood of 0 in X and f an analytic mapping of X0X_0 into X′X' such that f(0)=0f(0) = 0. Let f=f1+f2+f3+⋯f = f_1 + f_2 + f_3 + \cdots be the expansion of f as an integral series about 0, where fif_i is a homogeneous continuous-polynomial of degree i on X with values in X′X'. Let t be an element of TS2(X)^2(X), considered as a point distribution on X with support contained in \{0\}. Let t′=f∗(t)∈TS(X′)t' = f_*(t) \in TS(X'). The homogeneous component of t′t' of degree 1 is ⟨f2,t⟩\langle f_2, t \rangle.

Let t1′t'_1 be this component. Then, for every continuous linear mapping u of X′X' into a polynormed space,

u(t1′)=⟨t′,u⟩because u is continuous and linear u(t'_1) = \langle t', u \rangle \quad \text{because } u \text{ is continuous and linear}
=⟨t,u∘f⟩(Diff. & Anal. Man., R, 13.2.3) = \langle t, u \circ f \rangle \quad (\text{Diff. \& Anal. Man., R, 13.2.3})
=⟨t,u∘f2⟩because t∈TS2(X) = \langle t, u \circ f_2 \rangle \quad \text{because } t \in TS^2(X)
=u(⟨t,f2⟩)(Diff. & Anal. Man., R, 13.2.2), = u(\langle t, f_2 \rangle) \quad (\text{Diff. \& Anal. Man., R, 13.2.2}),

whence the lemma.

Proposition 24

Let G be a Lie group and (U,ϕ,E)(U, \phi, E) a chart on G such that ϕ(e)=0\phi(e) = 0. Let V be an open neighbourhood of e such that V2⊂UV^2 \subset U. Let m be the analytic mapping (a,b)↦ϕ(ϕ−1(a)ϕ−1(b))(a, b) \mapsto \phi(\phi^{-1}(a)\phi^{-1}(b)) of ϕ(V)×ϕ(V)\phi(V) \times \phi(V) into E. Let

m=∑i,j≥0mi,j m = \sum_{i, j \geq 0} m_{i, j}

be the expansion of m as an integral series about (0, 0), where mi,jm_{i,j} is a bihomogeneous continuous-polynomial of bidegree (i,j)(i, j) on E×EE \times E with values in EE.

(i) mi,0=m0,j=0m_{i,0} = m_{0,j} = 0 for all i≠1i \neq 1 and j≠1j \neq 1. (ii) m1,0(a,b)=am_{1,0}(a, b) = a and m0,1(a,b)=bm_{0,1}(a, b) = b for all a∈E,b∈Ea \in E, b \in E. (iii) *Let ψ:Te(G)→E\psi : T_e(G) \to E be the differential of ϕ\phi at e. For all u,vu, v in Te(G)T_e(G),

ψ([u,v])=m1,1(ψ(u),ψ(v))−m1,1(ψ(v),ψ(u)). \psi([u, v]) = m_{1,1}(\psi(u), \psi(v)) - m_{1,1}(\psi(v), \psi(u)).

m(a,0)=a, m(0,b)=bm(a, 0) = a,\ m(0, b) = b for all a,ba, b in ϕ(V)\phi(V), which proves (i) and (ii). Let u,vu, v be in Te(G)T_e(G). Let T0(E)T_0(E) be identified with EE and hence ψ\psi with Te(ϕ)T_e(\phi): The images of uu and vv under Te(ϕ)T_e(\phi) are ψ(u)\psi(u) and ψ(v)\psi(v). The tensor product point distribution of these images is the symmetric product of (ψ(u),0)(\psi(u), 0) and (0,ψ(v))(0, \psi(v)) in TS(E×E)=TS(E)×TS(E)TS(E \times E) = TS(E) \times TS(E), that is

(ψ(u),0)⊗(0,ψ(v))+(0,ψ(v))⊗(ψ(u),0). (\psi(u), 0) \otimes (0, \psi(v)) + (0, \psi(v)) \otimes (\psi(u), 0).

Hence ϕ∗(u∗v)\phi * (u * v) is the image of the above element under the mapping mm of ϕ(V)×ϕ(V)\phi(V) \times \phi(V) into EE. Its component of degree 1 in TS(E)TS(E) is, by Lemma 1,

x=⟨m1,1,(ψ(u),0)⊗(0,ψ(v))+(0,ψ(v))⊗(ψ(u),0)⟩. x = \langle m_{1,1}, (\psi(u), 0) \otimes (0, \psi(v)) + (0, \psi(v)) \otimes (\psi(u), 0) \rangle.

We define a bilinear mapping n:(E×E)2→En : (E \times E)^2 \to E by

n((a,b),(a′,b′))=m1,1(a,b′). n((a, b), (a', b')) = m_{1,1}(a, b').

Then n((a,b),(a,b))=m1,1(a,b)n((a, b), (a, b)) = m_{1,1}(a, b) and hence

x=⟨n,(ψ(u),0)⊗(0,ψ(v))+(0,ψ(v))⊗(ψ(u),0)⟩=m1,1(ψ(u),ψ(v))+m1,1(0,0)=m1,1(ψ(u),ψ(v)). x = \langle n, (\psi(u), 0) \otimes (0, \psi(v)) + (0, \psi(v)) \otimes (\psi(u), 0) \rangle \\ = m_{1,1}(\psi(u), \psi(v)) + m_{1,1}(0, 0) = m_{1,1}(\psi(u), \psi(v)).

Similarly, ϕ∗(v∗u)\phi * (v * u) admits m1,1(ϕ(v),ϕ(u))m_{1,1}(\phi(v), \phi(u)) as component of degree 1 in TS(E)TS(E). As ϕ([u,v])\phi([u, v]) is of degree 1, this proves (iii).

Corollary

The normable space Te(G)T_e(G) together with the bracket, is a normable Lie algebra.

Definition 6

The normable space Te(G)T_e(G), together with the bracket, is called the normable Lie algebra of G, or simply the Lie algebra of G, and is denoted by L(G)L(G).

Proposition 25

Let G be a Lie group and E(G)E(G) the enveloping algebra of L(G)L(G). The canonical injection of L(G)L(G) into E(G)E(G) defines a homomorphism θ\theta of the algebra E(G)E(G) into the algebra U(G)U(G). If K is of characteristic 0, η\eta is a bigebra isomorphism.

The bigebra U(G)U(G) is cocommutative (Differentiable and Analytic Manifolds, R, 13.5.1) and the filtration (Us(G))(U_s(G)) is compatible with the bigebra structure. The set of primitive elements of U(G)U(G) is L(G)L(G). It then suffices to apply chapter II, § 1, no. 6, Theorem 1.

When K is of characteristic 0 we shall in future identify U(G)U(G) with the enveloping algebra of L(G)L(G). By (2) and Proposition 7 (ii), the mapping t↦t∨t \mapsto t^\vee of U(G)U(G) into U(G)U(G) is then identified with the principal antiautomorphism of U(G)U(G) (Chapter I, § 2, no. 4).

Proposition 26

Suppose that K is of characteristic p>0p > 0. For all a∈L(G)a \in L(G), ap∈L(G)a^p \in L(G) and ad⁡(ap)=(ad⁡a)p\operatorname{ad}(a^p) = (\operatorname{ad} a)^p (the power apa^p being calculated in U(G)U(G)).

If a∈L(G)a \in L(G), aa is primitive in U(G)U(G), hence apa^p is primitive in U(G)U(G) (Chapter II, § 1, no. 2, Remark 1) and hence ap∈L(G)a^p \in L(G). Let σa\sigma_a (resp. τa\tau_a) be the linear mapping x↦a∗xx \mapsto a * x (resp. x↦x∗ax \mapsto x * a) of U(G)U(G) into U(G)U(G). For all x∈U(G)x \in U(G), (ad⁡a)(x)=(σa−τa)(x)(\operatorname{ad} a)(x) = (\sigma_a - \tau_a)(x) and hence (ad⁡a)p=(σa−τa)p(\operatorname{ad} a)^p = (\sigma_a - \tau_a)^p. But σa\sigma_a and τa\tau_a commute and therefore (σa−τa)p=(σa)p−(τa)p=τap−σap(\sigma_a - \tau_a)^p = (\sigma_a)^p - (\tau_a)^p = \tau_a^p - \sigma_a^p, whence the second assertion.

Definition 7

Let X be a manifold of class CrC^r (r≥2r \geq 2) and gg a complete normable Lie algebra. A law of infinitesimal left (resp. right) operation of class Cr−1C^{r-1} of gg on X is a mapping a↦Daa \mapsto D_a of gg into the set of vector fields on X with the following properties:

(a) the mapping (a,x)↦Da(x)(a, x) \mapsto D_a(x) is a morphism of class Cr−1C^{r-1} of the trivial vector bundle g×Xg \times X into the vector bundle T(X)T(X);

(b) [Da,Db]=−D[a,b][D_a, D_b] = -D_{[a, b]} (resp. [Da,Db]=D[a,b][D_a, D_b] = D_{[a, b]} for all a,ba, b in gg).

In particular, each vector field DaD_a is of class Cr−1C^{r-1}.

Remark

Let X be a manifold of class CrC^r, gg a finite-dimensional Lie algebra and a↦Daa \mapsto D_a a linear mapping of gg into the vector space of vector fields of class Cr−1C^{r-1} on X. Then condition (a) of Definition 7 holds. For, by considering a basis of gg and applying Differentiable and Analytic Manifolds, R, 7.7.1, the problem is reduced to the case dim⁡g=1\dim g = 1 and our assertion is then obvious.

Proposition 27

Let G be a Lie group and X a manifold of class CrC^r. Suppose that a law of left (resp. right) operation of class CrC^r of G on X is given. For all a∈L(G)a \in L(G), let DaD_a be the field of point distributions defined by a on X.

(i) The mapping (a,x)↦Da(x)(a, x) \mapsto D_a(x) is a morphism of class Cr−1C^{r-1} of the trivial vector bundle L(G)×XL(G) \times X into the vector bundle T(X)T(X).

(ii) Let I be an open subset of K containing 0 and γ:I→G\gamma : I \to G a mapping of class CrC^r such that γ(0)=e\gamma(0) = e. Let a=T0(γ)1∈L(G)a = T_0(\gamma)1 \in L(G). If f is a function of class CrC^r on an open subset of X, then

(Daf)(x)=lim⁡k∈K∗,k→0k−1(f(γ(k)x)−f(x))if G operates on the left, (D_a f)(x) = \lim_{k \in \mathbf{K}^*, k \to 0} k^{-1}(f(\gamma(k)x) - f(x)) \quad \text{if G operates on the left,}
(Daf)(x)=lim⁡k∈K∗,k→0k−1(f(xγ(k))−f(x))if G operates on the right. (D_a f)(x) = \lim_{k \in \mathbf{K}^*, k \to 0} k^{-1}(f(x\gamma(k)) - f(x)) \quad \text{if G operates on the right.}

(iii) If r≥2r \geq 2, the mapping a↦Daa \mapsto D_a is a law of infinitesimal left (resp. right) operation of class Cr−1C^{r-1} of L(G)L(G) on X.

Suppose that G operates on X on the left. Let ϕ:G×X→X\phi : G \times X \to X be the law of operation. Then T(ϕ)T(\phi) is a ϕ\phi-morphism of class Cr−1C^{r-1} of the vector bundle T(G)×T(X)T(G) \times T(X) into the vector bundle T(X)T(X) (Differentiable and Analytic

Manifolds, R, 8.1.2). The induced vector bundle (T(G)×T(X))∣{ϵ}×X(\mathrm{T}(G) \times \mathrm{T}(X))|_{\{\epsilon\} \times X} is identified with E=L(G)×T(X)E = L(G) \times T(X). Hence T(ϕ)∣ET(\phi)|E is a vector bundle morphism of class Cr−1C^{r-1}. For (a,x)∈L(G)×X,T(ϕ)(a,x)=Da(x)(a, x) \in L(G) \times X, T(\phi)(a, x) = D_a(x), whence (i).

The formula giving (Daf)(x)(D_a f)(x) follows from § 2, the end of no. 2, and Differentiable and Analytic Manifolds, R, 8.4.5.

Suppose that r⩾2r \geqslant 2. Let a,ba, b be in L(G)L(G) and ff be a function of class CrC^r on an open subset of XX. Then

D[a,b]f=Db(Daf)−Da(Dbf)by (17)=[Db,Da]f. \begin{align*} D_{[a, b]}f &= D_b(D_a f) - D_a(D_b f) \quad \text{by (17)} \\ &= [D_b, D_a]f \tag{Diff. \& Anal. Man., R, 8.5.3}. \end{align*}
Let x∈Xx \in X. By taking ff to be a chart on an open neighbourhood of xx, it follows that D[a,b](x)=[Db,Da](x)D_{[a, b]}(x) = [D_b, D_a](x), whence (iii). The argument is similar if GG operates on XX on the right.

When r⩾2r \geqslant 2, the mapping a↦Daa \mapsto D_a is called the law of infinitesimal operation associated with the given law of operation.

8. Functiorial properties of the Lie algebra

Let GG and HH be Lie groups and ϕ\phi a morphism of GG into HH. The restriction of U(ϕ)U(\phi) to L(G)L(G), which is just Te(ϕ)T_e(\phi), is a continuous morphism of L(G)L(G) into L(H)L(H), which we denote by L(ϕ)L(\phi). If ψ\psi is a morphism of HH into a Lie group, then L(ψ∘ϕ)=L(ψ)∘L(ϕ)L(\psi \circ \phi) = L(\psi) \circ L(\phi).

For ϕ\phi to be an immersion, it is necessary and sufficient that L(ϕ)L(\phi) be an isomorphism of L(G)L(G) onto a subalgebra of L(H)L(H) admitting a topological supplement. In particular, if GG is a Lie subgroup of HH and ϕ\phi is the canonical injection, L(G)L(G) is identified with a Lie subalgebra of L(H)L(H) by means of L(ϕ)L(\phi). More particularly, if GG is an open subgroup of HH, L(G)=L(H)L(G) = L(H).

If GG is a Lie quasi-subgroup of HH, L(G)L(G) is also identified with a closed Lie subgroup of L(H)L(H).

For ϕ\phi to be a submersion, it is necessary and sufficient that L(ϕ)L(\phi) be surjective and that its kernel admit a topological supplement. In that case, the kernel NN of ϕ\phi is a Lie subgroup of GG and L(N)=Ker⁡L(ϕ)L(N) = \operatorname{Ker} L(\phi). In particular, if HH is the quotient Lie group of GG by a normal Lie subgroup PP, L(P)L(P) is an ideal of L(G)L(G) and, if ϕ\phi is the canonical surjection of GG onto HH, L(G/P)L(G/P) is identified with L(G)/L(P)L(G)/L(P) by means of the morphism derived from L(ϕ)L(\phi) when passing to the quotient.

Let II be a finite set, (Gi)i∈I(G_i)_{i \in I} a family of Lie groups, GG their product and pip_i the canonical morphism of GG onto GiG_i. Then (L(pi))i∈I(L(p_i))_{i \in I} is a morphism of the Lie algebra L(G)L(G) into the Lie algebra ∏i∈IL(Gi)\prod_{i \in I} L(G_i) and is an isomorphism of normable spaces. L(G)L(G) is therefore identified with ∏i∈IL(Gi)\prod_{i \in I} L(G_i) by means of (L(pi))i∈I(L(p_i))_{i \in I}.

Proposition 28

Let G and H be Lie groups and φ a morphism of G into H. Suppose that K is of characteristic 0 and that H is finite-dimensional.

(i) The kernel N of φ is a Lie subgroup of G and L(N) = Ker L(φ).

(ii) The morphism ψ of G/N into H derived from φ when passing to the quotient is an immersion.

(iii) If φ(G) is closed in H and the topology of G has a countable base, φ(G) is a Lie subgroup of H, ψ is an isomorphism of the Lie group G/N onto the Lie group φ(G) and L(φ(G)) = Im L(φ).

Let G operate on H on the left by the mapping (g, h) ↦ φ(g)h. It suffices to apply Proposition 14 of § 1, no. 7, to the orbit of e.

Proposition 29

Let G and H be Lie groups and φ a morphism of G into H. Suppose that K is of characteristic 0 and that H is finite-dimensional. If H' is a Lie subgroup of H, then G' = φ⁻¹(H') is a Lie subgroup of G and L(G') = L(φ)⁻¹(L(H')).

Let π be the canonical mapping of H into the homogeneous space X = H/H'. Let G operate on X on the left by the mapping (g, x) ↦ φ(g)x. The stabilizer of π(e) is G', which is therefore a Lie subgroup of G (§ 1, no. 7, Proposition 14). The orbital mapping of π(e) is π ∘ φ. By Proposition 14 of § 1, L(G') is the kernel of L(π ∘ φ) = T_e(π) ∘ L(φ). The kernel of T_e(π) is L(H') (§ 1, no. 6, Proposition 11 (i)) and hence Ker L(π ∘ φ) = L(φ)⁻¹(L(H')).

Corollary 1

Let G, H be Lie groups and φ₁ and φ₂ morphisms of G into H. Suppose that K is of characteristic 0 and that H is finite-dimensional. The set of g ∈ G such that φ₁(g) = φ₂(g) is a Lie subgroup G' of G and L(G') is the set of x ∈ L(G) such that L(φ₁)x = L(φ₂)x.

We write φ(g) = (φ₁(g), φ₂(g)) for all g ∈ G, so that φ is a morphism of G into H × H. Let Δ be the diagonal subgroup of H × H. Then G' = φ⁻¹(Δ) and L(φ)x = (L(φ₁)x, L(φ₂)x) for all x ∈ L(G). It now suffices to apply Proposition 29.

Corollary 2

Let G be a finite-dimensional Lie group and G₁ and G₂ two Lie subgroups of G. Suppose that K is of characteristic 0. Then G₁ ∩ G₂ is a Lie subgroup of G with Lie algebra L(G₁) ∩ L(G₂).

We apply Proposition 29 to the canonical injection of G₁ into G and the subgroup G₂.

Corollary 3

Let G, G', H be Lie groups and φ : G → H and φ' : G' → H Lie group morphisms. Suppose that K is of characteristic 0 and that H is finite-dimensional. Let F be the set of (g, g') ∈ G × G' such that φ(g) = φ'(g'). Then F is a Lie subgroup of G × G' and L(F) is the set of (x, x') ∈ L(G) × L(G') such that L(φ)x = L(φ')x'.

We apply Corollary 1 to the morphisms (g, g') ↦ φ(g) and (g, g') ↦ φ'(g') of G × G' into H.

Proposition 30

Let G be a finite-dimensional Lie group with a countable base and

H and H' Lie subgroups of G. Suppose that K is of characteristic 0 and that HH' is locally closed in G.

(i) HH' is a submanifold of G and Te(HH′)=L(H)+L(H′)T_e(HH') = L(H) + L(H').

(ii) Suppose that every element of H commutes with every element of H'. Then HH' is a Lie subgroup of G. Let ϕ\phi be the mapping (h,h′)↦hh′(h, h') \mapsto hh' of H×H′H \times H' onto HH'. The kernel of ϕ\phi is the set of (m,m−1)(m, m^{-1}) where m∈H∩H′m \in H \cap H' and the morphism of (H×H′)/Ker ϕ(H \times H')/\mathrm{Ker}\ \phi onto HH' derived from ϕ\phi by passing to the quotient is a Lie group isomorphism.

Let H×H′H \times H' operate on G on the right by the mapping ((h,h′),g)↦hgh′−1((h, h'), g) \mapsto hg{h'}^{-1}. The orbital mapping ρ\rho of e is (h,h′)↦hh′−1(h, h') \mapsto h{h'}^{-1}. By Proposition 14 (iii) of § 1, no. 7, HH' is a submanifold of G and Te(HH′)=Im Te(ρ)T_e(HH') = \mathrm{Im}\ T_e(\rho). Now

Te(ρ)(L(H)×{0})=L(H)andTe(ρ)({0}×L(H′))=L(H′) T_e(\rho)(L(H) \times \{0\}) = L(H) \quad \text{and} \quad T_e(\rho)(\{0\} \times L(H')) = L(H')

and hence Te(HH′)=L(H)+L(H′)T_e(HH') = L(H) + L(H'). Suppose that every element of H commutes with every element of H'. Then HH' is a subgroup of G. By (i), it is a Lie subgroup of G. The rest of the statement follows from Proposition 28.

Proposition 31

Let G be a finite-dimensional Lie group with countable base, H a normal Lie subgroup of G and A a Lie subgroup of G. Suppose that K is of characteristic 0 and that AH is closed. Let ϕ\phi be the canonical morphism of G onto G/H. Then the canonical mappings

A/(H∩A)→ϕ(A),AH/H→ϕ(A) A/(H \cap A) \to \phi(A), \qquad AH/H \to \phi(A)

are Lie group isomorphisms.

By Proposition 30, AH is a Lie subgroup of G. By Corollary 2 to Proposition 29, H∩AH \cap A is a Lie subgroup of G. It is therefore meaningful to speak of the groups AH/HAH/H and A/(H∩A)A/(H \cap A). On the other hand, ϕ(A)\phi(A), which is the canonical image of AH in G/H, is closed and hence is a Lie subgroup of G/H (Proposition 28 (iii)). Proposition 28, applied to the composite morphisms A→G→G/HA \to G \to G/H and AH→G→G/HAH \to G \to G/H, proves that the canonical mappings of the proposition are Lie group isomorphisms.

Proposition 32

Let G and H be Lie groups, k a non-discrete closed subfield of K and ϕ\phi a morphism of G into H for the Lie group structures over k. Suppose that K is of characteristic 0. If L(ϕ)L(\phi) is K-linear, ϕ\phi is a morphism for the Lie group structures over K.

For all g∈Gg \in G,

Tg(ϕ)=Te(γ(ϕ(g)))∘L(ϕ)∘Tg(γ(g)−1) T_g(\phi) = T_e(\gamma(\phi(g))) \circ L(\phi) \circ T_g(\gamma(g)^{-1})

and hence Tg(ϕ)T_g(\phi) is K-linear. The proposition then follows from Differentiable and Analytic Manifolds, R, 5.14.6.

9. Lie algebra of the group of invertible elements of an algebra

Let AA be a complete normable associative algebra with unit element ee. Let A∗A^* be the group of invertible elements of AA. We have seen (§ 1, no. 1) that A∗A^* is an open submanifold of AA and is a Lie group. Let GG be a Lie group and ff a morphism of the Lie group GG into the Lie group A∗A^*. ff can be considered as an analytic mapping of GG into the complete normable space AA. Hence, if t∈T(∞)(G)t \in \mathscr{T}^{(\infty)}(G), we can form ⟨t,f⟩\langle t, f \rangle, which is an element of AA.

Proposition 33

The mapping t↦⟨t,f⟩t \mapsto \langle t, f \rangle is a morphism of the algebra T(∞)(G)\mathscr{T}^{(\infty)}(G) into the algebra AA.

It suffices to verify that, if tt and t′t' are point distributions on GG, then ⟨t∗t′,f⟩=⟨t,f⟩⟨t′,f⟩\langle t * t', f \rangle = \langle t, f \rangle \langle t', f \rangle. But

⟨t∗t′,f⟩=⟨t⊗t′,(g,g′)↦f(gg′)⟩=⟨t⊗t′,(g,g′)↦f(g)f(g′)⟩=⟨t,f⟩⟨t′,f⟩ \begin{align*} \langle t * t', f \rangle &= \langle t \otimes t', (g, g') \mapsto f(gg') \rangle \\ &= \langle t \otimes t', (g, g') \mapsto f(g)f(g') \rangle \\ &= \langle t, f \rangle \langle t', f \rangle \end{align*}
(Diff. & Anal. Man., R, 13.4.3).

The morphism of Proposition 33 is said to be associated with ff.

Take GG to be the group A∗A^* itself and ff to be the identity mapping ii of A∗A^*. We obtain a morphism, called canonical, of the algebra T(∞)(A∗)\mathscr{T}^{(\infty)}(A^*) into the algebra AA. The tangent space Te(A∗)T_e(A^*) is canonically identified with AA; and if t∈Te(A∗)t \in T_e(A^*), the definition of this identification is such that ⟨t,i⟩=t\langle t, i \rangle = t. Then Proposition 33 implies the following corollary:

Corollary

The canonical mapping ζ\zeta of L(A∗)L(A^*) into AA is an isomorphism of the Lie algebra, L(A∗)L(A^*) onto the Lie algebra AA. In other words,

ζ([a,b])=ζ(a)ζ(b)−ζ(b)ζ(a) \zeta([a, b]) = \zeta(a)\zeta(b) - \zeta(b)\zeta(a)
for all a,ba, b in L(A∗)L(A^*). If KK is of characteristic p>0p > 0, then ζ(ap)=ζ(a)p\zeta(a^p) = \zeta(a)^p for all a∈L(A∗)a \in L(A^*).

Henceforth L(A∗)L(A^*) and AA are identified by means of the isomorphism ζ\zeta.

The canonical morphism of T(∞)(A∗)\mathscr{T}^{(\infty)}(A^*) into AA has been obtained as a special case of the morphism of Proposition 33. But it is possible to argue in the opposite direction:

Proposition 34

Let HH be a Lie group, AA a unital complete normable associative algebra and ϕ:H→A∗\phi : H \to A^* a Lie group morphism. The associated morphism ϕ′\phi' of T(∞)(H)\mathscr{T}^{(\infty)}(H) into AA is obtained by composing ϕ∗\phi_* with the canonical morphism of T(∞)(A∗)\mathscr{T}^{(\infty)}(A^*) into AA. In particular, ϕ′(x)=L(ϕ)(x)\phi'(x) = L(\phi)(x) for all x∈L(H)x \in L(H).

Let ii be the identity mapping of A∗A^* into AA. Then, for all t∈T(∞)(H)t \in \mathscr{T}^{(\infty)}(H),

ϕ′(t)=⟨t,ϕ⟩=⟨t,i∘ϕ⟩=⟨ϕ∗(t),i⟩(Diff. & Anal. Man., R, 13.2.3). \begin{align*} \phi'(t) &= \langle t, \phi \rangle = \langle t, i \circ \phi \rangle \\ &= \langle \phi_*(t), i \rangle \quad \text{(Diff. \& Anal. Man., R, 13.2.3)}. \end{align*}

10. Lie algebras of certain linear groups

Let E be a complete normable space. Then L(E)\mathscr{L}(E) is a unital complete normable algebra and GL(E)\mathbf{GL}(E) is a Lie group. By the Corollary to Proposition 33, no. 9, if T1(GL(E))T_1(\mathbf{GL}(E)) is canonically identified with L(E)\mathscr{L}(E), the Lie algebra structure on L(GL(E))\mathbf{L}(\mathbf{GL}(E)) is given by the bracket (x,y)↦xy−yx(x, y) \mapsto xy - yx of two elements of L(E)\mathscr{L}(E). In particular, L(GL(n,K))\mathbf{L}(\mathbf{GL}(n, K)) is canonically identified with gl(n,K)\mathfrak{gl}(n, K) (Chapter I, § 1, no. 2).

Proposition 35

Let E be a finite-dimensional vector space. Let ϕ\phi be the morphism g↦det⁡gg \mapsto \det g of the Lie group GL(E)\mathbf{GL}(E) into the Lie group K∗K^*. The mapping L(ϕ)\mathbf{L}(\phi) of L(E)\mathscr{L}(E) into K is the mapping x↦Tr⁡xx \mapsto \operatorname{Tr} x. The kernel SL(E)\mathbf{SL}(E) of ϕ\phi is a Lie subgroup of GL(E)\mathbf{GL}(E) with Lie algebra sl(E)\mathfrak{sl}(E).

We choose a norm and a basis of E. The expansion of the determinant proves that

det⁡(1+u)∈1+Tr⁡u+o(∥u∥) \det(1 + u) \in 1 + \operatorname{Tr} u + o(\|u\|)
when uu tends to 0 in L(E)\mathscr{L}(E). Hence, using Proposition 34, no. 9, for x∈L(E)=L(GL(E))x \in \mathscr{L}(E) = \mathbf{L}(\mathbf{GL}(E)):
L(ϕ)(x)=⟨x,ϕ⟩=Tr⁡x. \mathbf{L}(\phi)(x) = \langle x, \phi \rangle = \operatorname{Tr} x.
It follows that ϕ\phi is a submersion. Therefore, Ker⁡ϕ=SL(E)\operatorname{Ker} \phi = \mathbf{SL}(E) is a Lie subgroup of GL(E)\mathbf{GL}(E) whose Lie algebra is Ker⁡L(ϕ)=sl(E)\operatorname{Ker} \mathbf{L}(\phi) = \mathfrak{sl}(E).

Let E1,…,EnE_1, \ldots, E_n be complete normable spaces and E their direct sum. Every x∈L(E)x \in \mathscr{L}(E) can be represented by a matrix (xij)1≤i,j≤n(x_{ij})_{1 \leq i, j \leq n}, where xij∈L(Ei,Ej)x_{ij} \in \mathscr{L}(E_i, E_j).

Proposition 36

Let I be a subset of {1,2,…,n}\{1, 2, \ldots, n\} and G the subgroup of GL(E)\mathbf{GL}(E) consisting of the g=(gij)1≤i,j≤n∈GL(E)g = (g_{ij})_{1 \leq i, j \leq n} \in \mathbf{GL}(E) such that gij=0g_{ij} = 0 for i<ji < j and gii=1g_{ii} = 1 for i∈Ii \in I. Then G is a Lie subgroup of GL(E)\mathbf{GL}(E) and L(G)\mathbf{L}(G) is the set of x=(xij)1≤i,j≤n∈L(E)x = (x_{ij})_{1 \leq i, j \leq n} \in \mathscr{L}(E) such that xij=0x_{ij} = 0 for i<ji < j and xii=0x_{ii} = 0 for i∈Ii \in I.

Let S be the set of (xij)∈L(E)(x_{ij}) \in \mathscr{L}(E) such that xij=0x_{ij} = 0 for i<ji < j and xii=0x_{ii} = 0 for i∈Ii \in I. Then G is the intersection of GL(E)\mathbf{GL}(E) and the affine subspace 1+S1 + S of L(E)\mathscr{L}(E). Hence G is a submanifold of GL(E)\mathbf{GL}(E) and the tangent space to G at 1 is identified with S.

In particular, in GL(n,K)\mathbf{GL}(n, K), the total lower triangular subgroup and the lower strict triangular subgroup, defined as in Integration, Chapter VII, § 3, no. 3, are Lie subgroups with Lie algebras t(n,K)t(n, K) and n(n,K)n(n, K) (Chapter I, § 1, no. 2).

Proposition 37

Let A be a complete normable unital associative algebra and x↦xtx \mapsto x^t a continuous linear mapping of A into A such that (xt)t=x(x^t)^t = x and (xy)t=ytxt(xy)^t = y^t x^t for all x,yx, y in A. Suppose that K is of characteristic ≠2\neq 2. Let G be the subgroup of A∗A^* consisting of the x∈Ax \in A such that xxt=xtx=1xx^t = x^t x = 1. Then G is a Lie subgroup of A∗A^* and L(G)\mathbf{L}(G) is the set of y∈Ay \in A such that yt=−yy^t = -y.

Let S (resp. S') be the set of y∈Ay \in A such that y=yty = y^t (resp. y=−yty = -y^t). Then S, S' are closed vector subspaces of A. The formula

y=12(y+yt)+12(y−yt) y = \frac{1}{2}(y + y^t) + \frac{1}{2}(y - y^t)

proves that A is the topological direct sum of S and S'. Let f be the mapping of A into S defined by f(x)=xxtf(x) = xx^t. This mapping is analytic. For all y∈Ay \in A, f(1+y)=1+y+yt+yytf(1 + y) = 1 + y + y^t + yy^t; choose a norm on A compatible with its algebra structure; then

f(1+y)∈1+y+yt+o(∥y∥)for y tending to 0. f(1 + y) \in 1 + y + y^t + o(\|y\|) \quad \text{for } y \text{ tending to } 0.

Thus, T1(f)(y)=y+ytT_1(f)(y) = y + y^t, so that f is a submersion at 1. Therefore, there exists an open neighbourhood U of 1 in A such that U∩GU \cap G is a submanifold of U. Hence (§ 1, no. 3, Proposition 6) G is a Lie subgroup of A*. Moreover, L(G)=Te(G)=Ker⁡T1(f)L(G) = T_e(G) = \operatorname{Ker} T_1(f).

Corollary 1

Suppose that K is of characteristic ≠2\neq 2. Let E be a finite-dimensional vector space over K and ϕ\phi a non-degenerate symmetric (resp. alternating) bilinear form on E. For all u∈L(E)u \in \mathscr{L}(E), let u∗u^* be the adjoint of u relative to ϕ\phi. Let G be the orthogonal (resp. symplectic) group of ϕ\phi. Then G is a Lie subgroup of GL(E)\mathbf{GL}(E) and L(G)L(G) is the set of x∈L(E)x \in \mathscr{L}(E) such that x∗=−xx^* = -x.

We apply Proposition 37 with A=L(E)A = \mathscr{L}(E) and xt=x∗x^t = x^*.

Remark

Let B be a basis of E and J the matrix of ϕ\phi with respect to B. Then L(G)L(G) is the set of elements of L(E)\mathscr{L}(E) whose matrix X with respect to B satisfies the equation

tX=−JXJ−1. {}^tX = -JXJ^{-1}.

This follows from Algebra, Chapter IX, § 1, formula (50).

Corollary 2

Let E be a complex (resp. real) Hilbert space and U the unitary group of E. Then U is a real subgroup of GL(E)\mathbf{GL}(E) and L(U)L(U) is the set of x∈L(E)x \in \mathscr{L}(E) such that x∗=−xx^* = -x.

We apply Proposition 37 with A=L(E)A = \mathscr{L}(E) considered as an algebra over R\mathbf{R} and xt=x∗x^t = x^*.

Corollary 3

Let E be a finite-dimensional complex vector space, ϕ\phi a non-degenerate Hermitian sesquilinear form on E and U the unitary group of ϕ\phi. Then U is a real Lie subgroup of GL(E)\mathbf{GL}(E) and L(U)L(U) is the set of x∈L(E)x \in \mathscr{L}(E) such that ixix is Hermitian.

When E≠{0}E \neq \{0\}, U is not a Lie subgroup of the complex Lie group GL(E)\mathbf{GL}(E), for L(U)L(U) is not a complex vector subspace of L(E)\mathscr{L}(E).

11. Linear representations

Let G be a Lie group, E a complete normable space and π\pi an analytic linear representation of G on E (§ 1, no. 2). The associated morphism t↦⟨t,π⟩t \mapsto \langle t, \pi \rangle of T(∞)(G)\mathscr{T}^{(\infty)}(G) into L(E)\mathscr{L}(E) is an algebra morphism (no. 9, Proposition 33) and its restriction to L(G)L(G) is L(π)L(\pi). Hence L(π)L(\pi) is a representation of L(G)L(G) on EE (Chapter I, § 3, Definition 1).

Proposition 38

Consider GG as operating on EE on the left by the mapping (g,x)↦π(g)x(g, x) \mapsto \pi(g)x. Let b∈Eb \in E and φ(b)\varphi(b) be its orbital mapping. Let Tb(E)T_b(E) be canonically identified with EE. For all t∈L(G)t \in L(G),

(L(π)t)(b)=⟨t,φ(b)⟩=φ(b)∗t=t∗εb. (L(\pi)t)(b) = \langle t, \varphi(b) \rangle = \varphi(b)*t = t * \varepsilon_b.

In particular, the vector field defined by tt on EE is the field b↦(L(π)t)(b)b \mapsto (L(\pi)t)(b).

L(π)t=⟨t,π⟩L(\pi)t = \langle t, \pi \rangle (no. 9, Proposition 34). As the mapping A↦AbA \mapsto Ab of L(E)\mathscr{L}(E) into EE is continuous and linear, it follows that

(L(π)t)(b)=⟨t,g↦π(g)b⟩=⟨t,IdE∘φ(b)⟩=⟨φ(b)∗t,IdE⟩(Diff. & Anal. Man., R, 13.2.3)=φ(b)∗t. \begin{align*} (L(\pi)t)(b) &= \langle t, g \mapsto \pi(g)b \rangle \\ &= \langle t, \mathrm{Id}_E \circ \varphi(b) \rangle \\ &= \langle \varphi(b)*t, \mathrm{Id}_E \rangle \quad (\text{Diff. \& Anal. Man., R, 13.2.3}) \\ &= \varphi(b)*t. \end{align*}

Finally, φ(b)∗t=t∗εb\varphi(b)*t = t * \varepsilon_b (no. 3, Proposition 14 (ii)).

Proposition 39

Suppose that KK is of characteristic 0. Let GG be a Lie group, EE a finite-dimensional vector space and π\pi an analytic linear representation of GG on EE. Let E1,E2E_1, E_2 be vector subspaces of EE such that E2⊂E1E_2 \subset E_1. The set G1G_1 of g∈Gg \in G such that π(g)x≡x\pi(g)x \equiv x (mod. E2E_2) for all x∈E1x \in E_1 is a Lie subgroup of GG and L(G1)L(G_1) is the set of a∈L(G)a \in L(G) such that L(π)aL(\pi)a maps E1E_1 into E2E_2.

This follows from Propositions 29 (no. 8) and 36 (no. 10).

Corollary 1

In the notation of Proposition 39, the set of g∈Gg \in G such that π(g)(E1)⊂E1\pi(g)(E_1) \subset E_1 is a Lie subgroup of GG and its Lie algebra is the set of a∈L(G)a \in L(G) such that L(π)aL(\pi)a maps E1E_1 into E1E_1.

We apply Proposition 39 with E1=E2E_1 = E_2.

Corollary 2

Let G,E,πG, E, \pi be as in Proposition 39. Let FF be a subset of EE. The set of g∈Gg \in G such that π(g)x=x\pi(g)x = x for all x∈Fx \in F is a Lie subgroup of GG and its Lie algebra is the set of a∈L(G)a \in L(G) such that (L(π)a)(x)=0(L(\pi)a)(x) = 0 for all x∈Fx \in F.

We apply Proposition 39 with E2={0}E_2 = \{0\} and E1E_1 the vector subspace of EE generated by FF.

Let π1,π2,…,πn\pi_1, \pi_2, \ldots, \pi_n be analytic linear representations of GG. Clearly the direct sum π\pi of the πi\pi_i (Algebra, Chapter VIII, § 13, no. 1) is an analytic linear representation of GG and L(π)L(\pi) is the direct sum of L(π1),L(π2),…,L(πn)L(\pi_1), L(\pi_2), \ldots, L(\pi_n) (Chapter I, § 3, no. 1).

Proposition 40

Let GG be a Lie group, EE a complete normable space, π\pi an analytic linear representation of GG on EE and FF a closed vector subspace of EE stable under π(G)\pi(G). Suppose that KK is of characteristic 0, or that FF is a direct factor of EE.

(i) The subrepresentation π1\pi_1 and the quotient representation π2\pi_2 of π\pi defined by FF are analytic representations.

(ii) FF is stable under L(π)(L(G))L(\pi)(L(G)).

(iii) Let ϱ1\varrho_1 and ϱ2\varrho_2 be the subrepresentation and quotient representation of L(π)L(\pi) defined by FF. Then L(π1)=ϱ1,L(π2)=ϱ2L(\pi_1) = \varrho_1, L(\pi_2) = \varrho_2.

Let AA be the set of u∈L(E)u \in \mathscr{L}(E) such that u(F)⊂Fu(F) \subset F. Then AA is a closed vector subspace of L(E)\mathscr{L}(E) and π\pi takes its values in AA. By virtue of the hypotheses on KK and FF, the mapping π′:G→A\pi': G \to A with the same graph as π\pi is analytic (Differentiable and Analytic Manifolds, R, 5.8.5). The canonical mappings θ1:A→L(F)\theta_1 : A \to \mathscr{L}(F) and θ2:A→L(E/F)\theta_2 : A \to \mathscr{L}(E/F) are continuous and linear and hence analytic. This proves (i). The mappings Te(π)T_e(\pi) and Te(π′)T_e(\pi') have the same graph and hence L(π)(L(G))⊂AL(\pi)(L(G)) \subset A, which proves (ii). We have

Te(π1)=Te(θ1∘π′)=θ1∘Te(π′)=ϱ1Te(π2)=Te(θ2∘π′)=θ2∘Te(π′)=ϱ2. T_e(\pi_1) = T_e(\theta_1 \circ \pi') = \theta_1 \circ T_e(\pi') = \varrho_1 \\ T_e(\pi_2) = T_e(\theta_2 \circ \pi') = \theta_2 \circ T_e(\pi') = \varrho_2.

Proposition 41

Let* GG be a Lie group and π1,π2,…,πn,π\pi_1, \pi_2, \ldots, \pi_n, \pi analytic linear representation of GG on complete normable spaces E1,E2,…,En,EE_1, E_2, \ldots, E_n, E. Let

(x1,x2,…,xn)↦x1x2…xn (x_1, x_2, \ldots, x_n) \mapsto x_1 x_2 \ldots x_n
be a continuous multilinear mapping of E1×E2×⋯×EnE_1 \times E_2 \times \cdots \times E_n into EE. Suppose that
π(g)(x1x2…xn)=(π1(g)x1)(π2(g)x2)…(πn(g)xn) \pi(g)(x_1 x_2 \ldots x_n) = (\pi_1(g)x_1)(\pi_2(g)x_2) \ldots (\pi_n(g)x_n)
for all g∈G,x1∈E1,…,xn∈Eng \in G, x_1 \in E_1, \ldots, x_n \in E_n. Then
(L(π)a)(x1x2…xn)=∑i=1nx1x2…xi−1((L(πi)a)xi)xi+1…xn (L(\pi)a)(x_1 x_2 \ldots x_n) = \sum_{i=1}^n x_1 x_2 \ldots x_{i-1} ((L(\pi_i)a)x_i) x_{i+1} \ldots x_n
for all a∈L(G),x1∈E1,…,xn∈Ena \in L(G), x_1 \in E_1, \ldots, x_n \in E_n.

As an example we perform the calculation for n=2n = 2.

(L(π)a)(x1x2)=⟨a,g↦π(g)(x1x2)⟩(Proposition 38)=⟨a,(g↦π1(g)x1)(g↦π2(g)x2)⟩=⟨a,g↦π1(g)x1⟩⋅x2+x1⋅⟨a,g↦π2(g)x2⟩(*Diff.* & *Anal.* *Man.*, R, 5.5.6)=((L(π1)a)x1)⋅x2+x1⋅((L(π2)a)x2)(Proposition 38). \begin{align*} (L(\pi)a)(x_1 x_2) &= \langle a, g \mapsto \pi(g)(x_1 x_2) \rangle & \text{(Proposition 38)} \\ &= \langle a, (g \mapsto \pi_1(g)x_1)(g \mapsto \pi_2(g)x_2) \rangle \\ &= \langle a, g \mapsto \pi_1(g)x_1 \rangle \cdot x_2 + x_1 \cdot \langle a, g \mapsto \pi_2(g)x_2 \rangle & \text{(*Diff.* \& *Anal.* *Man.*, R, 5.5.6)} \\ &= ((L(\pi_1)a)x_1) \cdot x_2 + x_1 \cdot ((L(\pi_2)a)x_2) & \text{(Proposition 38)}. \end{align*}

Corollary 1

Let* GG be a Lie group, E1,…,En+1E_1, \ldots, E_{n+1} complete normable spaces and π1,…,πn+1\pi_1, \ldots, \pi_{n+1} analytic linear representations of GG on E1,…,En+1E_1, \ldots, E_{n+1}. Let

E=L(E1,…,En;En+1) E = \mathscr{L}(E_1, \ldots, E_n; E_{n+1})
the complete normable space of continuous multilinear mappings of E1×⋯×EnE_1 \times \cdots \times E_n into En+1E_{n+1} (General Topology, Chapter X, § 3, no. 2). For all g∈Gg \in G, let π(g)\pi(g) be the automorphism of EE defined by
(π(g)u)(x1,…,xn)=πn+1(g)(u(π1(g)−1x1,…,πn(g)−1xn)). (\pi(g)u)(x_1, \ldots, x_n) = \pi_{n+1}(g)(u(\pi_1(g)^{-1}x_1, \ldots, \pi_n(g)^{-1}x_n)).

Then π\pi is an analytic linear representation of GG on EE and

((L(π)a)u)(x1,…,xn)=−∑i=1nu(x1,…,xi−1,(L(πi)a)xi,xi+1,…,xn) ((L(\pi)a)u)(x_1, \ldots, x_n) = -\sum_{i=1}^n u(x_1, \ldots, x_{i-1}, (L(\pi_i)a)x_i, x_{i+1}, \ldots, x_n)
+(L(πn+1)a)(u(x1,…,xn)) \quad + (L(\pi_{n+1})a)(u(x_1, \ldots, x_n))
for all a∈L(G)a \in L(G), u∈Eu \in E, x1∈E1,…,xn∈Enx_1 \in E_1, \ldots, x_n \in E_n.

Every element (A1,…,An+1)(A_1, \ldots, A_{n+1}) of L(E1)×⋯×L(En+1)\mathscr{L}(E_1) \times \cdots \times \mathscr{L}(E_{n+1}) defines a continuous endomorphism θ(A1,…,An+1)\theta(A_1, \ldots, A_{n+1}) of EE by the formula

(θ(A1,…,An+1)u)(x1,…,xn)=An+1(u(A1x1,…,Anxn)). (\theta(A_1, \ldots, A_{n+1})u)(x_1, \ldots, x_n) = A_{n+1}(u(A_1x_1, \ldots, A_nx_n)).
The mapping θ\theta of L(E1)×⋯×L(En+1)\mathscr{L}(E_1) \times \cdots \times \mathscr{L}(E_{n+1}) into L(E)\mathscr{L}(E) is continuous and multilinear. Then, for all g∈Gg \in G,
π(g)=θ(π1(g−1),…,πn(g−1),πn+1(g)) \pi(g) = \theta(\pi_1(g^{-1}), \ldots, \pi_n(g^{-1}), \pi_{n+1}(g))
and hence π\pi is analytic. We apply Proposition 41 to the mapping
(x1,…,xn,u)↦u(x1,…,xn) (x_1, \ldots, x_n, u) \mapsto u(x_1, \ldots, x_n)
of E1×⋯×En×EE_1 \times \cdots \times E_n \times E into En+1E_{n+1}. Then
πn+1(g)(u(x1,…,xn))=(π(g)u)(π1(g)x1,…,πn(g)xn) \pi_{n+1}(g)(u(x_1, \ldots, x_n)) = (\pi(g)u)(\pi_1(g)x_1, \ldots, \pi_n(g)x_n)
and hence
(L(πn+1)a)(u(x1,…,xn))=∑i=1nu(x1,…,(L(πi)a)xi,…,xn) (L(\pi_{n+1})a)(u(x_1, \ldots, x_n)) = \sum_{i=1}^n u(x_1, \ldots, (L(\pi_i)a)x_i, \ldots, x_n)
+((L(π)a)u)(x1,…,xn). \quad + ((L(\pi)a)u)(x_1, \ldots, x_n).

When the EiE_i are finite-dimensional, the representation L(π)L(\pi) of L(G)L(G) is derived from the representations L(π1),…,L(πn+1)L(\pi_1), \ldots, L(\pi_{n+1}) under the procedure of Chapter I, § 3, Proposition 3.

Corollary 2

Let GG be a Lie group and π\pi an analytic linear representation of GG on a complete normable space EE. Then g↦tπ(g)−1g \mapsto {}^t\pi(g)^{-1} is an analytic linear representation ρ\rho of GG on the complete normable space L(E,K)\mathscr{L}(E, K)\footnote{As when K=RK = \mathbf{R} or C\mathbf{C}, the transpose tπ(g){}^t\pi(g) considered here is the restriction to L(E,K)\mathscr{L}(E, K) of the transpose of π(g)\pi(g) in the purely algebraic sense.} and L(ρ)a=−t(L(π)a)L(\rho)a = -{}^t(L(\pi)a) for all a∈L(G)a \in L(G).

This is a special case of Corollary 1.

ρ\rho is called the contragredient representation of π\pi.

When EE is finite-dimensional, L(ρ)L(\rho) is the dual representation of L(π)L(\pi) in the sense of Chapter I, § 3, no. 3.

Corollary 3

Let GG be a Lie group and π1,…,πn\pi_1, \ldots, \pi_n analytic linear representations of GG on finite-dimensional vector spaces E1,…,EnE_1, \ldots, E_n. Then the representation π1⊗⋯⊗πn\pi_1 \otimes \cdots \otimes \pi_n of GG (Appendix) is analytic and L(π1⊗⋯⊗πn)L(\pi_1 \otimes \cdots \otimes \pi_n) is the tensor product of L(π1),…,L(πn)L(\pi_1), \ldots, L(\pi_n).

The mapping (A1,…,An)↦A1⊗⋯⊗An(A_1, \ldots, A_n) \mapsto A_1 \otimes \cdots \otimes A_n of L(E1)×⋯×L(En)\mathscr{L}(E_1) \times \cdots \times \mathscr{L}(E_n) into L(E1⊗⋯⊗En)\mathscr{L}(E_1 \otimes \cdots \otimes E_n) is multilinear, whence the fact that π\pi is analytic. Consider the mapping (x1,…,xn)↦x1⊗⋯⊗xn(x_1, \ldots, x_n) \mapsto x_1 \otimes \cdots \otimes x_n of E1×⋯×EnE_1 \times \cdots \times E_n into

E1⊗⋯⊗En. E_1 \otimes \cdots \otimes E_n.
By Proposition 41, we see that
(L(π)a)(x1⊗⋯⊗xn)=∑i=1nx1⊗⋯⊗(L(πi)a)xi⊗⋯⊗xn (L(\pi)a)(x_1 \otimes \cdots \otimes x_n) = \sum_{i=1}^n x_1 \otimes \cdots \otimes (L(\pi_i)a)x_i \otimes \cdots \otimes x_n
for all a∈L(G)a \in L(G), xi∈Eix_i \in E_i for 1≤i≤n1 \leq i \leq n. Hence L(π)L(\pi) is the tensor product of the L(πi)L(\pi_i).

Corollary 4

Let GG be a Lie group and π\pi an analytic linear representation of GG on a finite-dimensional vector space EE. Then the representations Tn(π)T^n(\pi), Sn(π)S^n(\pi) and ∧n(π)\wedge^n(\pi) of GG (Appendix) are analytic and

L(Tn(π))=Tn(L(π)),L(Sn(π))=Sn(L(π)),L(∧n(π))=∧n(L(π)). L(T^n(\pi)) = T^n(L(\pi)), \quad L(S^n(\pi)) = S^n(L(\pi)), \quad L(\wedge^n(\pi)) = \wedge^n(L(\pi)).
This follows from Corollary 3 and Proposition 40.

Corollary 5

Let AA be a finite-dimensional algebra. Suppose that KK is of characteristic 0. The automorphism group Aut(A)\mathrm{Aut}(A) of AA is a Lie subgroup of GL(A)\mathbf{GL}(A) and L(Aut(A))L(\mathrm{Aut}(A)) is the Lie algebra of derivation of AA.

This follows from Corollary 1 (applied to E=L(A,A;A)E = \mathscr{L}(A, A; A)) and Corollary 2 of Proposition 39 (applied to the subset of EE consisting only of multiplication on AA).

Remark

We apply Corollary 1 with G=GL(F)G = \mathbf{GL}(F) (FF a complete normable space), π1=π2=IdG\pi_1 = \pi_2 = \mathrm{Id}_G and π3\pi_3 the trivial representation of GG on KK. We obtain an analytic representation π\pi of GL(F)\mathbf{GL}(F) on L(F,F;K)\mathscr{L}(F, F; K). We assume that FF is finite-dimensional and that KK is of characteristic 0. Applying Corollary 2 to Proposition 39 to π\pi, we recover part of Corollary 1 to Proposition 37.

Proposition 42

Let GG be a Lie group, XX an analytic manifold, (g,x)↦gx(g, x) \mapsto gx (resp. xgxg) a law of analytic left (resp. right) operation of GG on XX and x0x_0 a point of XX which is invariant under GG. For all g∈Gg \in G, let τ(g)\tau(g) be the automorphism x↦gxx \mapsto gx (resp. xgxg) of XX and let π(g)\pi(g) be the automorphism of Tx0(X)T_{x_0}(X) tangent at x0x_0 to τ(g)\tau(g). (i) π\pi is an analytic representation of GG (resp. G∨G^\vee) on Tx0(X)T_{x_0}(X). (ii) For all a∈L(G)a \in L(G) and all ξ0∈Tx0(X)\xi_0 \in T_{x_0}(X), L(π)a.ξ0L(\pi)a.\xi_0 can be calculated as follows: let DaD_a be the vector field defined by aa on XX and ξ\xi a vector field of class C1C^1 in an open neighbourhood of x0x_0 such that ξ(x0)=ξ0\xi(x_0) = \xi_0; then

L(π)a.ξ0=−[Da,ξ](x0). L(\pi)a.\xi_0 = -[D_a, \xi](x_0).

τ(gg′)=τ(g)τ(g′)\tau(gg') = \tau(g)\tau(g') (resp. τ(g′)τ(g)\tau(g')\tau(g)) and hence π(gg′)=π(g)π(g′)\pi(gg') = \pi(g)\pi(g') (resp. π(g′)π(g)\pi(g')\pi(g)). On the other hand, since TXTX is a vector G-bundle of class CωC^\omega (§ 1, no. 8, Proposition 16), π\pi is analytic, whence (i).

To prove (ii), suppose that G operates on the left. There exists an open neighbourhood I of 0 in K and an analytic mapping γ\gamma of I into G such that γ(0)=e,T0(γ)1=a\gamma(0) = e, T_0(\gamma)1 = a. Then DaD_a is the vector field on X defined by the mapping ϕ:(λ,x)↦γ(λ)x\phi : (\lambda, x) \mapsto \gamma(\lambda)x of I×XI \times X into X (§ 2, no. 2). If ϕλ\phi_\lambda denotes the bijection x↦γ(λ)xx \mapsto \gamma(\lambda)x of X into X, then

[Da,ξ](x0)=(ddλ(Tϕλ(x0)(ϕλ−1)ξ(ϕλ(x0))))λ=0(Diff. & Anal. Man., R, [D_a, \xi](x_0) = \left( \frac{d}{d\lambda} (T_{\phi_\lambda(x_0)}(\phi_\lambda^{-1})\xi(\phi_\lambda(x_0))) \right)_{\lambda=0} \quad (\text{Diff. \& Anal. Man., R,}
=(ddλ(Tx0(ϕλ−1)ξ0))λ=0 = \left( \frac{d}{d\lambda} (T_{x_0}(\phi_\lambda^{-1})\xi_0) \right)_{\lambda=0}
=(ddλ(π(γ(λ))−1ξ0))λ=0. = \left( \frac{d}{d\lambda} (\pi(\gamma(\lambda))^{-1}\xi_0) \right)_{\lambda=0}.

As the mappings λ↦γ(λ)−1\lambda \mapsto \gamma(\lambda)^{-1} and λ↦γ(−λ)\lambda \mapsto \gamma(-\lambda) are tangent at 0, this is also equal to

−(ddλ(π(γ(λ))ξ0))λ=0 - \left( \frac{d}{d\lambda} (\pi(\gamma(\lambda))\xi_0) \right)_{\lambda=0}
=−(ddλ(π∘γ)(λ))λ=0ξ0 = - \left( \frac{d}{d\lambda} (\pi \circ \gamma)(\lambda) \right)_{\lambda=0} \xi_0
=−L(π)a.ξ0. = -L(\pi)a.\xi_0.

12. Adjoint representation

Let G be a Lie group. Consider the law of analytic left operation

(g,g′)↦gg′g−1=(Int⁡g)g′ (g, g') \mapsto gg'g^{-1} = (\operatorname{Int} g)g'
of G into G. This law of operation defines, by no. 3, a bilinear mapping of T(∞)(G)×T(∞)(G)\mathscr{T}^{(\infty)}(G) \times \mathscr{T}^{(\infty)}(G) into T(∞)(G)\mathscr{T}^{(\infty)}(G), which we shall denote by τ\tau in this no. By Proposition 13 of no. 3,
(t∗t′)τt′′=tτ(t′τt′′) (t * t') \tau t'' = t \tau (t' \tau t'')
for all t,t′,t′′t, t', t'' in T(∞)(G)\mathscr{T}^{(\infty)}(G). By Proposition 14 (i) of no. 3,
εgτt=(Int⁡g)∗t \varepsilon_g \tau t = (\operatorname{Int} g)_*t
for all g∈Gg \in G and t∈T(∞)(G)t \in \mathscr{T}^{(\infty)}(G). In particular, the mapping t↦εgτtt \mapsto \varepsilon_g \tau t of T(∞)(G)\mathscr{T}^{(\infty)}(G) into T(∞)(G)\mathscr{T}^{(\infty)}(G) is an automorphism of the bigebra T(∞)(G)\mathscr{T}^{(\infty)}(G). Its restrictions to U(G),Us(G),L(G)U(G), U_s(G), L(G) are denoted by Ad⁡U(G)(g),Ad⁡Us(G)(g),Ad⁡L(G)(g)\operatorname{Ad}_{U(G)}(g), \operatorname{Ad}_{U_s(G)}(g), \operatorname{Ad}_{L(G)}(g). We often write Ad⁡(g)\operatorname{Ad}(g) instead of Ad⁡L(G)(g)\operatorname{Ad}_{L(G)}(g) when no confusion is possible. By (23), Ad⁡(g)\operatorname{Ad}(g) is the tangent mapping at e to Int⁡(g)\operatorname{Int}(g). It is an automorphism of the normable

Lie algebra L(G)\mathbf{L}(G). When KK is of characteristic 0, AdU(G)(g)\mathrm{Ad}_{\mathbf{U}(G)}(g) is the unique automorphism of U(G)\mathbf{U}(G) which extends Ad(g)\mathrm{Ad}(g).

If ϕ\phi is a morphism of the Lie group GG into a Lie group HH, then

ϕ∗(t⊤t′)=ϕ∗(t)⊤ϕ∗(t′) \phi_*(t \top t') = \phi_*(t) \top \phi_*(t')
for all t,t′t, t' in T(∞)(G)\mathscr{T}^{(\infty)}(G); this follows from Proposition 15 of no. 3.

Proposition 43

Let t,ut, u be in T(∞)(G)\mathscr{T}^{(\infty)}(G). Let ∑i=1nti⊗ti′\sum_{i=1}^n t_i \otimes t'_i be the image of tt under the coproduct. Then*

t⊤u=∑i=1nti∗u∗ti′∨. t \top u = \sum_{i=1}^n t_i * u * {t'_i}^\vee.

By definition, t⊤ut \top u is the image of t⊗ut \otimes u under the mapping (g,g′)↦gg′g−1(g, g') \mapsto gg'g^{-1} of G×GG \times G into GG. Now this mapping is obtained by composing the following mappings:

α:(g,g′)↦(g,g,g′)of G×G into G×G×Gβ:(g,g′,g′′)↦(g,g′−1,g′′)of G×G×G into G×G×Gγ:(g,g′,g′′)↦gg′′g′of G×G×G into G. \begin{aligned} \alpha & : (g, g') \mapsto (g, g, g') & \text{of } G \times G \text{ into } G \times G \times G \\ \beta & : (g, g', g'') \mapsto (g, {g'}^{-1}, g'') & \text{of } G \times G \times G \text{ into } G \times G \times G \\ \gamma & : (g, g', g'') \mapsto gg''g' & \text{of } G \times G \times G \text{ into } G. \end{aligned}

On the other hand:

α∗(t⊗u)=∑i=1n(ti⊗ti′)⊗u=∑i=1nti⊗ti′⊗uβ∗(∑i=1nti⊗ti′⊗u)=∑i=1nti⊗ti′∨⊗uγ∗(∑i=1nti⊗ti′∨⊗u)=∑i=1nti∗u∗ti′∨. \begin{aligned} \alpha_*(t \otimes u) &= \sum_{i=1}^n (t_i \otimes t'_i) \otimes u = \sum_{i=1}^n t_i \otimes t'_i \otimes u \\ \beta_* \left( \sum_{i=1}^n t_i \otimes t'_i \otimes u \right) &= \sum_{i=1}^n t_i \otimes {t'_i}^\vee \otimes u \\ \gamma_* \left( \sum_{i=1}^n t_i \otimes {t'_i}^\vee \otimes u \right) &= \sum_{i=1}^n t_i * u * {t'_i}^\vee. \end{aligned}

Corollary 1

Let u∈L(G)u \in \mathbf{L}(G) and u′∈T(∞)(G)u' \in \mathscr{T}^{(\infty)}(G). Then u⊤u′=u∗u′−u′∗uu \top u' = u * u' - u' * u.

The image of uu under the coproduct is u⊗εe+εe⊗uu \otimes \varepsilon_e + \varepsilon_e \otimes u, whence

u⊤u′=u∗u′∗εe+εe∗u′∗u∨=u∗u′−u′∗u. u \top u' = u * u' * \varepsilon_e + \varepsilon_e * u' * u^\vee = u * u' - u' * u.

Corollary 2

Let t∈T(∞)(G)t \in \mathscr{T}^{(\infty)}(G) and g∈Gg \in G. Then εg⊤t=εg∗t∗εg−1\varepsilon_g \top t = \varepsilon_g * t * \varepsilon_{g^{-1}}. If t∈L(G)t \in \mathbf{L}(G), then εg⊤t=gtg−1\varepsilon_g \top t = gtg^{-1} (where the latter product is evaluated in the group T(G)\mathbf{T}(G)).

The image of εg\varepsilon_g under the coproduct is εg⊗εg\varepsilon_g \otimes \varepsilon_g.

Corollary 3

Let a∈L(G)a \in \mathbf{L}(G). The vector field defined by aa and the left operation g↦Int gg \mapsto \mathrm{Int}\, g of GG on GG is the field Ra−La\mathbf{R}_a - \mathbf{L}_a.

The value of this field at gg is

a⊤εg=a∗εg−εg∗a(Corollary 1)=(Ra)g−(La)g(Definition 5). \begin{aligned} a \top \varepsilon_g &= a * \varepsilon_g - \varepsilon_g * a & \text{(Corollary 1)} \\ &= (\mathbf{R}_a)_g - (\mathbf{L}_a)_g & \text{(Definition 5)}. \end{aligned}

For all g∈Gg \in G and all t∈L(G)t \in L(G),

(Ad g)(t)=εg⊤t=εg∗t∗εg−1=gtg−1. (\mathrm{Ad}\,g)(t) = \varepsilon_g \top t = \varepsilon_g * t * \varepsilon_g^{-1} = gtg^{-1}.
Since Ad g=Te(Int g)\mathrm{Ad}\,g = T_e(\mathrm{Int}\,g), Proposition 42 of no. 11 proves that Ad\mathrm{Ad} is an analytic linear representation of GG on the normable space L(G)L(G).

Definition 8

The representation Ad of G on L(G) is called the adjoint representation of G.

Proposition 44

For all a∈L(G)a \in L(G),*

(L(Ad))(a)=adL(G)a. (L(\mathrm{Ad}))(a) = \mathrm{ad}_{L(G)}a.
Let b∈L(G)b \in L(G). By Proposition 42 (ii) of no. 11 and Corollary 3 to Proposition 43,
(L(Ad))(a).b=−[Ra−La1Lb](e). (L(\mathrm{Ad}))(a).b = -[R_a - L_{a_1}L_b](e).
Now Ra∘Lb=Lb∘RaR_a \circ L_b = L_b \circ R_a (no. 6, Proposition 23 (ii)), whence [Ra,Lb]=0[R_a, L_b] = 0; then, using Proposition 23 (ii),
(L(Ad))(a).b=[La,Lb](e)=L[a,b](e)=[a,b]=(adL(G)a)b. (L(\mathrm{Ad}))(a).b = [L_a, L_b](e) = L_{[a, b]}(e) = [a, b] = (\mathrm{ad}_{L(G)}a)b.

Proposition 45

Suppose that G is finite-dimensional and that K is of characteristic 0. Let s be an integer ⩾0\geqslant 0. Then the mapping π:g↦AdUs(G)(g)\pi : g \mapsto \mathrm{Ad}_{U_s(G)}(g) is an analytic linear representation of G on Us(G)U_s(G) and L(π)a=adUs(G)aL(\pi)a = \mathrm{ad}_{U_s(G)}a for all a∈L(G)a \in L(G).

The linear representation π\pi is a quotient of ⨁r=0sTr(Ad)\bigoplus_{r=0}^s \mathrm{Tr}(\mathrm{Ad}) and is hence analytic. For a∈L(G)a \in L(G) and x1,x2,…,xsx_1, x_2, \ldots, x_s in L(G)L(G),

(L(π)a)(x1x2…xs)=∑i=1sx1…(L(Ad)a.xi)…xs(Proposition 41)=∑i=1sx1…([a,xi])…xs(Proposition 44)=(AdUs(G)a)(x1x2…xs). \begin{align*} (L(\pi)a)(x_1x_2\ldots x_s) &= \sum_{i=1}^s x_1 \ldots (L(\mathrm{Ad})a.x_i) \ldots x_s & \text{(Proposition 41)} \\ &= \sum_{i=1}^s x_1 \ldots ([a, x_i]) \ldots x_s & \text{(Proposition 44)} \\ &= (\mathrm{Ad}_{U_s(G)}a)(x_1x_2\ldots x_s). \end{align*}

Proposition 46

Let h∈G,x∈Th(G)h \in G, x \in T_h(G) and a∈L(G)a \in L(G). Let ϕ\phi be the mapping (g,g′)↦gg′g−1(g, g') \mapsto gg'g^{-1} of G×GG \times G into GG. The image y of (a,x)∈Te(G)×Th(G)(a, x) \in T_e(G) \times T_h(G) under T(e,h)(ϕ)T_{(e, h)}(\phi) is y=x+h((Ad h−1)a−a)y = x + h((\mathrm{Ad}\,h^{-1})a - a). We have*

y=(T(e,h)ϕ)(a⊗εh+εe⊗x)=a⊤εh+εe⊤x=a∗εh−εh∗a+x=h((Ad h−1)a)−ha+x. \begin{align*} y &= (T_{(e, h)}\phi)(a \otimes \varepsilon_h + \varepsilon_e \otimes x) \\ &= a \top \varepsilon_h + \varepsilon_e \top x \\ &= a * \varepsilon_h - \varepsilon_h * a + x \\ &= h((\mathrm{Ad}\,h^{-1})a) - ha + x. \end{align*}

Proposition 47

Let G be a Lie group, H and E Lie subgroups of G and suppose that hEh−1^{-1} = E for all h \in H. Then T(∞)(H)⊂T(∞)(E)⊂T(∞)(E)\mathscr{T}^{(\infty)}(H) \subset \mathscr{T}^{(\infty)}(E) \subset \mathscr{T}^{(\infty)}(E). In particular, Ad(H)(L(E))⊂L(E)\mathrm{Ad}(H)(L(E)) \subset L(E) and [L(H),L(E)]⊂L(E)[L(H), L(E)] \subset L(E).

If t∈T(∞)(H)t \in \mathscr{T}^{(\infty)}(H) and t′∈T(∞)(E)t' \in \mathscr{T}^{(\infty)}(E), then t⊗t′∈T(∞)(H×E)t \otimes t' \in \mathscr{T}^{(\infty)}(H \times E) and the image of H×EH \times E under the mapping (g,g′)↦gg′g−1(g, g') \mapsto gg'g^{-1} is contained in E.

Proposition 48

Let G be a Lie group and H and E Lie subgroups of G. Suppose that G is, as a Lie group, the semi-direct product of H by E. Let φ\varphi be the linear representation g↦(Ad g)∣L(E)g \mapsto (\mathrm{Ad}\, g) \mid L(E) of the Lie group G on L(E)L(E) (cf. Proposition 47) and let σ\sigma be the restriction of φ\varphi to H. Then: (i) L(G)L(G) is the topological direct sum of L(H)L(H) and L(E)L(E); (ii) L(H)L(H) is a subalgebra of L(G)L(G) and L(E)L(E) is an ideal of L(G)L(G); (iii) L(σ)L(\sigma) is a linear representation of L(H)L(H) on the Lie algebra of derivations of L(E)L(E); (iv) L(G)L(G) is the semi-direct product of L(H)L(H) by L(E)L(E) defined by L(σ)L(\sigma) (Chapter I, § 1, no. 8).

(i) is obvious and (ii) follows from Proposition 47. L(σ)=L(φ)∣L(H)L(\sigma) = L(\varphi) \mid L(H). Now by Propositions 40 (no. 11) and 44 (no. 12), L(φ)(t)L(\varphi)(t) is, for all t∈L(G)t \in L(G), the restriction of adL(G)t\mathrm{ad}_{L(G)} t to L(E)L(E). This proves (iii). Using (i) and (ii), this also proves (iv).

Corollary

Let G be a Lie group. Let Te(G)T_e(G) be given its unique commutative Lie algebra structure. Let τ\tau be an adjoint representation of L(G)L(G). Then the Lie algebra of T(G)T(G) is the semi-direct product of L(G)L(G) by Te(G)T_e(G) defined by τ\tau. In other words, for x,x′x, x' in L(G)L(G) and y,y′y, y' in Te(G)T_e(G),

[(x,y),(x′,y′)]=([x,x′],[x,y′]+[y,x′]) [(x, y), (x', y')] = ([x, x'], [x, y'] + [y, x'])

(where the bracket on the left is evaluated in L(T(G))L(T(G)) and the brackets on the right in L(G)L(G)).

This follows from Proposition 48 and Proposition 6 of § 2, no. 2.

Proposition 49

Let A be a complete normable unital associative algebra. We identify A with L(A∗)L(A^*). Then, if g∈A∗g \in A^* and y∈Ay \in A, (Ad g)y=gyg−1(\mathrm{Ad}\, g)y = gyg^{-1}.

Recall that Ad g=T1(Int g)\mathrm{Ad}\, g = T_1(\mathrm{Int}\, g). Let ugu_g be the mapping x↦gxg−1x \mapsto gxg^{-1} of A into A. The identity chart of A∗A^* into A transforms Int g\mathrm{Int}\, g into ug∣A∗u_g \mid A^*. The tangent mapping at each point of A∗A^* to this mapping is equal to ugu_g, whence the proposition.

Corollary

For all g∈A∗g \in A^*, let i(g)i(g) be the automorphism y↦gyg−1y \mapsto gyg^{-1} of A, so that ii is an analytic linear representation of A∗A^* on A. For all z∈L(A∗)=A,L(i)zz \in L(A^*) = A, L(i)z is the inner derivation y↦zy−yzy \mapsto zy - yz of A.

This follows from Propositions 49 and 44.

13. Tensors and invariant forms

Let G be a Lie group. We consider G as operating on itself by left (resp. right) translation. Let λ\lambda be a vector functor of class CωC^\omega for isomorphisms. Then λ(TG)\lambda(\mathrm{TG}) is an analytic left (resp. right) vector G-bundle (§ 1, no. 8, Corollary to Proposition 16). The mapping (g,u)↦gu(g, u) \mapsto gu (resp. ugug) of G×λ(L(G))G \times \lambda(\mathrm{L}(G)) onto λ(TG)\lambda(\mathrm{TG}) is an isomorphism ϕ\phi (resp. ψ\psi) of vector G-bundles (§ 7, no. 8, Corollary 2 to Proposition 17). Every G-invariant section of λ(TG)\lambda(\mathrm{TG}) is analytic and determined by its value at ee (§ 1, no. 8, Corollary 1 to Proposition 17). Such a section is called left (resp. right) invariant. Let σ\sigma be a left invariant section of λ(TG)\lambda(\mathrm{TG}); the transform σ′\sigma' of σ\sigma under a right translation δ(g)\delta(g) is defined by σ′(δ(g)h)=λ(Th(δ(g)))σ(h)\sigma'(\delta(g)h) = \lambda(\mathrm{T}_h(\delta(g)))\sigma(h) for all h∈Gh \in G; it is also left invariant; it is also derived from σ\sigma by γ(g)∘δ(g)=Int(g)\gamma(g) \circ \delta(g) = \mathrm{Int}(g) and hence

σ′(e)=λ(Ad g)⋅σ(e). \sigma'(e) = \lambda(\mathrm{Ad}\ g)\cdot \sigma(e).

Similarly, let τ\tau be a right invariant section of λ(TG)\lambda(\mathrm{TG}); the transform τ′\tau' of τ\tau under a left translation γ(g)\gamma(g) is also right variant and

τ′(e)=λ(Ad g)⋅τ(e). \tau'(e) = \lambda(\mathrm{Ad}\ g)\cdot \tau(e).

We now consider G×GG \times G as operating on GG on the left by

((g,g′),g′′)↦gg′′g′−1. ((g, g'), g'') \mapsto gg''{g'}^{-1}.

Then G is a left Lie homogeneous space of G×GG \times G (§ 1, no. 6, Example). Hence λ(TG)\lambda(\mathrm{TG}) is an analytic left vector (G×G)(G \times G)-bundle. A section of λ(TG)\lambda(\mathrm{TG}) is called biinvariant if it is invariant under the action of G×GG \times G on λ(TG)\lambda(\mathrm{TG}), in other words if it is invariant under left and right translations. Let λ(L(G))0\lambda(\mathrm{L}(G))_0 be the set of elements of λ(L(G))\lambda(\mathrm{L}(G)) invariant under λ(Ad(G))\lambda(\mathrm{Ad}(G)). For all u∈λ(L(G))0u \in \lambda(\mathrm{L}(G))_0, let σu\sigma_u be the mapping of GG into λ(TG)\lambda(\mathrm{TG}) defined by σu(g)=gu=ug\sigma_u(g) = gu = ug. Then u↦σuu \mapsto \sigma_u is a bijection of λ(L(G))0\lambda(\mathrm{L}(G))_0 onto the set of biinvariant sections of λ(TG)\lambda(\mathrm{TG}) (§ 1, no. 8, Corollary 1 to Proposition 17).

Proposition 50

Let G be a Lie Group (assumed to be finite-dimensional if K is of characteristic > 0). Let E be the vector space of continuous alternating multilinear forms of degree k on Te(G)\mathrm{T}_e(G). For all u∈Eu \in E, let ωu\omega^u be the differential form of degree k on G such that (ωu)g(\omega^u)_g is the multilinear form on Tg(G)\mathrm{T}_g(G) derived from u by the translation h↦ghh \mapsto gh (resp. h↦hgh \mapsto hg). Then ωu\omega^u is analytic and left (resp. right) invariant on G. The mapping u↦ωuu \mapsto \omega^u is an isomorphism of E onto the vector space of left (resp. right) invariant differential forms of degree k on G.

This is a special case of what we have said above.

Let F be a complete normable space. Proposition 50 remains true if differential forms on G with values in K are replaced by differential forms on G with values in F. For every continuous linear mapping uu of Te(G)\mathrm{T}_e(G) into F, there exists a differential form ωu\omega^u of degree 1 on G, with values in F, such that (ωu)g=u∘Tg(γ(g)−1)(\omega^u)_g = u \circ \mathrm{T}_g(\gamma(g)^{-1}). In particular, take F=Te(G)F = \mathrm{T}_e(G) and u=IdTe(G)u = \mathrm{Id}_{\mathrm{T}_e(G)}. We then obtain the differential form ω\omega on GG such that ωg=Tg(γ(g−1))\omega_g = T_g(\gamma(g^{-1})); this differential form is left invariant and analytic; it is called the left canonical differential form of GG. ωg(t)=g−1t\omega_g(t) = g^{-1}t for all t∈Tg(G)t \in T_g(G).

If FF is again an arbitrary complete normable space and u∈L(Te(G),F)u \in \mathscr{L}(T_e(G), F), then ωu=u∘ω\omega^u = u \circ \omega. In particular (taking F=KF = K), the mapping v↦v∘ωv \mapsto v \circ \omega is a linear bijection of the dual of Te(G)T_e(G) onto the vector space of differential forms of degree 1 with values in KK which are left invariant under GG.

Similarly, the differential form ω′\omega' on GG such that ωg′=Tg(δ(g))\omega'_g = T_g(\delta(g)) is called the right canonical differential form of GG. There are analogous properties to those of ω\omega, which we leave to the reader to state. The mapping g↦g−1g \mapsto g^{-1} of GG onto GG transforms ω\omega into ω′\omega'.

14. Maurer–cartan formulae

Let XX be a manifold of class CrC^r, of finite dimension if KK is of characteristic >0> 0, and let LL be a complete normable Lie algebra. Let α\alpha be a differential form of degree 1 on XX with values in LL of class Cr−1C^{r-1}. Let x∈Xx \in X. The mapping

(u1,u2)↦[αx(u1),αx(u2)] (u_1, u_2) \mapsto [\alpha_x(u_1), \alpha_x(u_2)]

of Tx(X)×Tx(X)T_x(X) \times T_x(X) into LL is a continuous alternating bilinear form on Tx(X)T_x(X) with values in LL. We shall denote it by [α]x2[\alpha]^2_x, so that [α]2[\alpha]^2 is a differential form of degree 2 on XX with values in LL. Identifying an open neighbourhood of xx in XX with an open subset of a Banach space, we see immediately that [α]2[\alpha]^2 is of class Cr−1C^{r-1}. If X′X' is a manifold of class CrC^r and f:X′→Xf : X' \to X is a morphism, then

[f∗(α)]2=f([α]2). [f^*(\alpha)]^2 = f([\alpha]^2).

Let α,β\alpha, \beta be two differential forms of degree 1 on XX with values in LL of class Cr−1C^{r-1}. The exterior product α∧β\alpha \wedge \beta of α\alpha and β\beta (Differentiable and Analytic Manifolds, R, 7.8.2) is a differential form of degree 2 on XX with values in LL of class Cr−1C^{r-1}; we have

(α∧β)x(u1,u2)=[αx(u1),βx(u2)]−[αx(u2),βx(u1)] (\alpha \wedge \beta)_x(u_1, u_2) = [\alpha_x(u_1), \beta_x(u_2)] - [\alpha_x(u_2), \beta_x(u_1)]

for u1,u2u_1, u_2 in Tx(X)T_x(X). It is immediate that

[α+β]2=[α]2+[β]2+α∧β [\alpha + \beta]^2 = [\alpha]^2 + [\beta]^2 + \alpha \wedge \beta
α∧α=2[α]2. \alpha \wedge \alpha = 2[\alpha]^2.

Proposition 51

Let GG be a Lie group, of finite dimension if KK is of characteristic >0> 0, and let a1,…,apa_1, \ldots, a_p be elements of L(G)L(G), FF a complete normable space and α\alpha a differential form of degree p−1p-1 on GG with values in FF. If α\alpha is left invariant, then

(dα)e(a1,…,ap)=∑i<j(−1)i+jαe([ai,aj],a1,…,ai−1,ai+1,…,aj−1,aj+1,…,ap). (d\alpha)_e(a_1, \ldots, a_p) = \sum_{i<j} (-1)^{i+j} \alpha_e([a_i, a_j], a_1, \ldots, a_{i-1}, a_{i+1}, \ldots, a_{j-1}, a_{j+1}, \ldots, a_p).

If α\alpha is right invariant, then

(dα)e(a1,…,ap)=−∑i<j(−1)i+jαe([ai,aj],a1,…,ai−1,ai+1,…,aj−1,aj+1,…,ap). (d\alpha)_e(a_1, \ldots, a_p) = - \sum_{i < j} (-1)^{i+j} \alpha_e([a_i, a_j], a_1, \ldots, a_{i-1}, a_{i+1}, \ldots, a_{j-1}, a_{j+1}, \ldots, a_p).
Suppose that α\alpha is left invariant. By Differentiable and Analytic Manifolds, R, 8.5.7, then
(dα)(La1,…,Lap)=∑i(−1)i−1Laiα(La1,…,Lai−1,Lai+1,…,Lap)+∑i<j(−1)i+jα([Lai,Laj],La1,…,Lai−1,Lai+1,…,Laj−1,Laj+1,…,Lap). (d\alpha)(L_{a_1}, \ldots, L_{a_p}) = \sum_i (-1)^{i-1} L_{a_i} \alpha(L_{a_1}, \ldots, L_{a_{i-1}}, L_{a_{i+1}}, \ldots, L_{a_p}) + \sum_{i < j} (-1)^{i+j} \alpha([L_{a_i}, L_{a_j}], L_{a_1}, \ldots, L_{a_{i-1}}, L_{a_{i+1}}, \ldots, L_{a_{j-1}}, L_{a_{j+1}}, \ldots, L_{a_p}).
But the functions α(La1,…,Lai−1,Lai+1,…,Lap)\alpha(L_{a_1}, \ldots, L_{a_{i-1}}, L_{a_{i+1}}, \ldots, L_{a_p}) on G are left invariant and therefore constant. Hence
Laiα(La1,…,Lai−1,Lai+1,…,Lap)=0. L_{a_i} \alpha(L_{a_1}, \ldots, L_{a_{i-1}}, L_{a_{i+1}}, \ldots, L_{a_p}) = 0.
Moreover, [Lai,Laj]=L[ai,aj][L_{a_i}, L_{a_j}] = L_{[a_i, a_j]} (Proposition 23), whence the first formula of Proposition 51. The second can be established analogously, this time using the relation [Rai,Raj]=−R[ai,aj][R_{a_i}, R_{a_j}] = -R_{[a_i, a_j]}.

Corollary 1

Let G be a Lie group, of finite dimension if K is of characteristic > 0, and ω\omega and ω′\omega' the left and right canonical differential forms of G. Then*

dω+[ω]2=0,dω′−[ω′]2=0. d\omega + [\omega]^2 = 0, \qquad d\omega' - [\omega']^2 = 0.
By Proposition 51,
(dω)e(a1,a2)=−ωe([a1,a2])=−[a1,a2]=−[ωe(a1),ωe(a2)]=−[ω]e2(a1,a2) (d\omega)_e(a_1, a_2) = -\omega_e([a_1, a_2]) = -[a_1, a_2] = -[\omega_e(a_1), \omega_e(a_2)] = -[\omega]^2_e(a_1, a_2)
whence the first formula. The second can be established analogously.

Corollary 2

Suppose that G is finite-dimensional. Let (e1,…,en)(e_1, \ldots, e_n) be a basis of L(G)L(G), (e1∗,…,en∗)(e_1^*, \ldots, e_n^*) the dual basis, (cijk)(c_{ijk}) the constants of structure of L(G)L(G) relative to the basis (e1,…,en)(e_1, \ldots, e_n) and ωi\omega_i (resp. ωi′\omega'_i) the left (resp. right) invariant differential form on G with values in K such that (ωi)e=ei∗(\omega_i)_e = e_i^* (resp. (ωi′)e=ei∗(\omega'_i)_e = e_i^*). Then*

dωk+∑i<jcijkωi∧ωj=0(k=1,2,…,n) d\omega_k + \sum_{i < j} c_{ijk} \omega_i \wedge \omega_j = 0 \quad (k = 1, 2, \ldots, n)
dωk′−∑i<jcijkωi′∧ωj′=0(k=1,2,…,n). d\omega'_k - \sum_{i < j} c_{ijk} \omega'_i \wedge \omega'_j = 0 \quad (k = 1, 2, \ldots, n).
If r<sr < s,
(dωk)e(er,es)=−(ωk)e([er,es])=−∑icrsi(ωk)e(ei)=−crsk=−∑i<jcijk(ωi∧ωj)e(er,es). (d\omega_k)_e(e_r, e_s) = -(\omega_k)_e([e_r, e_s]) = -\sum_i c_{rsi} (\omega_k)_e(e_i) = -c_{rsk} = -\sum_{i < j} c_{ijk} (\omega_i \wedge \omega_j)_e(e_r, e_s).
The argument is similar for the ωk′\omega'_k.

15. Construction of invariant differential forms

Lemma 2

Let G be a Lie group, U a symmetric open neighbourhood of e in G, E a complete normable space and ϕ:U2→E\phi : U^2 \to E an analytic mapping. For all g∈Ug \in U, let ωg\omega_g be the differential at the point g of the mapping h↦ϕ(g−1h)h \mapsto \phi(g^{-1}h). Then ω\omega is the restriction to U of the left invariant differential form on G whose value at e is deϕd_e \phi.

Clearly ωe=deϕ\omega_e = d_e \phi. For all g∈Ug \in U and all t∈Te(G)t \in T_e(G),

⟨ωg,Te(γ(g))t⟩=⟨dg(ϕ∘γ(g)−1),Te(γ(g))t⟩=⟨deϕ∘Tg(γ(g)−1),Te(γ(g))t⟩=⟨deϕ,t⟩ \langle \omega_g, T_e(\gamma(g))t \rangle = \langle d_g(\phi \circ \gamma(g)^{-1}), T_e(\gamma(g))t \rangle \\ = \langle d_e \phi \circ T_g(\gamma(g)^{-1}), T_e(\gamma(g))t \rangle = \langle d_e \phi, t \rangle

and hence ωg\omega_g is derived from deϕd_e \phi by Te(γ(g))T_e(\gamma(g)).

Proposition 52

Let n be an integer > 0, G an n-dimensional Lie group, U a symmetric open neighbourhood of e in G and ψ:U2→Kn\psi : U^2 \to K^n a chart of G such that ψ(e)=0\psi(e) = 0. If (x1,…,xn)(x_1, \ldots, x_n) are the coordinates of x∈ψ(U)x \in \psi(U) and (y1,…,yn)(y_1, \ldots, y_n) the coordinates of y∈ψ(U)y \in \psi(U), we denote by

m1(x1,…,xn,y1,…,yn),…,mn(x1,…,xn,y1,…,yn) m_1(x_1, \ldots, x_n, y_1, \ldots, y_n), \ldots, m_n(x_1, \ldots, x_n, y_1, \ldots, y_n)

the coordinates of ψ(ψ−1(x)−1ψ−1(y))\psi(\psi^{-1}(x)^{-1}\psi^{-1}(y)). Then, if we write, for 1≤k≤n1 \leq k \leq n,

ϖk(x1,…,xn)=Dn+1mk(x1,…,xn,x1,…,xn)dx1+⋯+D2nmk(x1,…,xn,x1,…,xn)dxn, \varpi_k(x_1, \ldots, x_n) = D_{n+1} m_k(x_1, \ldots, x_n, x_1, \ldots, x_n) dx_1 + \cdots \\ + D_{2n} m_k(x_1, \ldots, x_n, x_1, \ldots, x_n) dx_n,

the differential forms ϖk\varpi_k on ψ(U)\psi(U) are derived through ψ\psi from left invariant differential forms on G and are such that ϖk(0,…,0)=dxk\varpi_k(0, \ldots, 0) = dx_k.

We apply Lemma 2 with E=KE = K, taking ϕ(g)\phi(g) to be the coordinate of ψ(g)\psi(g) of index k. We obtain a differential form ωk\omega_k; let ϖk\varpi_k be its transform under ψ\psi. The value of ϖk\varpi_k at (x1,…,xn)(x_1, \ldots, x_n) is the differential at (x1,…,xn)(x_1, \ldots, x_n) of the function y↦mk(x1,…,xn,y1,…,yn)y \mapsto m_k(x_1, \ldots, x_n, y_1, \ldots, y_n); this value is therefore given by formula (32). It then suffices to use the conclusion to Lemma 2.

Proposition 53

Let G be a Lie group, A a complete normable algebra and ϕ\phi a Lie group morphism of G into A∗A^*. For all g∈Gg \in G, let ωg=ϕ(g)−1dgϕ\omega_g = \phi(g)^{-1} d_g \phi. Then ω\omega is the left invariant differential form on G whose value at e is deϕd_e \phi.

We apply Lemma 2 with E=AE = A and U=GU = G. The differential at g of the mapping h↦ϕ(g−1h)=ϕ(g)−1ϕ(h)h \mapsto \phi(g^{-1}h) = \phi(g)^{-1} \phi(h) is ϕ(g)−1dgϕ\phi(g)^{-1} d_g \phi.

16. Haar measure on a Lie group

Let G be a Lie group of finite dimension n. Then ⋀n(Te(G))\bigwedge^n(T_e(G)) is of dimension 1. Hence (no. 13) the vector space S of left invariant differential forms of degree n on G is of dimension 1. Let (ω1,…,ωn)(\omega_1, \ldots, \omega_n) be a basis of the space of left invariant differential forms of degree 1 on G; then ω1∧ω2∧⋯∧ωn\omega_1 \wedge \omega_2 \wedge \cdots \wedge \omega_n is a basis of S.

Proposition 54

Let G be a Lie group of finite dimension n, ω a left invariant differential form of degree n on G and φ an endomorphism of G. Then

ϕ∗(ω)=(det⁡L(ϕ))ω. \phi^*(\omega) = (\det L(\phi)) \omega.

We write L(ϕ)=uL(\phi) = u, ωe=f\omega_e = f and ϕ∗(ω)e=g\phi^*(\omega)_e = g. For all x1,…,xnx_1, \ldots, x_n in L(G)L(G),

g(x1,…,xn)=f(ux1,…,uxn)=(det⁡u)f(x1,…,xn) g(x_1, \ldots, x_n) = f(ux_1, \ldots, ux_n) = (\det u)f(x_1, \ldots, x_n)

and hence ϕ∗(ω)e=det⁡L(ϕ)⋅ωe\phi^*(\omega)_e = \det L(\phi) \cdot \omega_e. On the other hand, if g∈Gg \in G,

ϕ∘γ(g)=γ(ϕ(g))∘ϕ \phi \circ \gamma(g) = \gamma(\phi(g)) \circ \phi

and hence γ(g)∗ϕ∗(ω)=ϕ∗(ω)\gamma(g)^*\phi^*(\omega) = \phi^*(\omega). Thus ϕ∗(ω)\phi^*(\omega) is left invariant, whence the proposition.

Corollary

For all g∈Gg \in G,

δ(g)∗ω=(det⁡Ad g)ω. \delta(g)^*\omega = (\det \mathrm{Ad}\, g) \omega.
δ(g)∗ω=δ(g)∗γ(g)∗ω=(Int g)∗ω and L(Int g)=Ad g. \delta(g)^*\omega = \delta(g)^*\gamma(g)^*\omega = (\mathrm{Int}\, g)^*\omega \text{ and } L(\mathrm{Int}\, g) = \mathrm{Ad}\, g.

Let G be a locally compact group and φ an endomorphism of G. Suppose that there exist open neighbourhoods V, V′V' of e such that ϕ(V)=V′\phi(V) = V' and ϕ∣V\phi|V is a local isomorphism of G into G. Let μ be a left Haar measure on G. By Integration, Chapter VII, § 1, Corollary to Proposition 9, there exists a unique number a>0a > 0 such that ϕ(μ∣V)=a−1μ∣V′\phi(\mu|V) = a^{-1}\mu|V'. Clearly a is independent of the choice of V, V′V' and μ. It is called the modulus of φ and is denoted by modGϕ\mathrm{mod}_G \phi or simply mod ϕ\mathrm{mod}\, \phi. When φ is an automorphism of G, we recover Definition 4 of Integration, Chapter VII, § 1.

Proposition 55

Suppose that K is locally compact. Let μ be a Haar measure on the additive group of K. Let G be a Lie group of finite dimension n.

(i) Let ω be a non-zero left invariant differential form of degree n on G. Then the measure mod(ω)μ\mathrm{mod}(\omega)_\mu (Differentiable and Analytic Manifolds, R, 10.1.6) is a left Haar measure on G. If K=RK = \mathbf{R} and G has the orientation defined by ω, the measure defined by ω (Differentiable and Analytic Manifolds, R, 10.4.3) is a left Haar measure on G.

(ii) Let φ be an étale endomorphism of G. Then mod ϕ=mod det⁡L(ϕ)\mathrm{mod}\, \phi = \mathrm{mod}\, \det L(\phi).

(i) is obvious. Let V, V′V' be open neighbourhoods of e such that ϕ(V)=V′\phi(V) = V' and ϕ∣V\phi|V is a local isomorphism of G into G. Then

ϕ−1(mod(ω)μ∣V′)=mod(ϕ∗(ω))μ∣V)by transport of structure \phi^{-1}(\mathrm{mod}(\omega)_\mu|V') = \mathrm{mod}(\phi^*(\omega))_\mu|V) \quad \text{by transport of structure}
=mod(det⁡L(ϕ)ω∣V)μ(Proposition 54) = \mathrm{mod}(\det L(\phi)\omega|V)_\mu \quad \text{(Proposition 54)}
=mod det⁡L(ϕ)(mod(ω)μ∣V) = \mathrm{mod}\, \det L(\phi)(\mathrm{mod}(\omega)_\mu|V)

whence mod ϕ=mod det⁡L(ϕ)\mathrm{mod}\, \phi = \mathrm{mod}\, \det L(\phi) by definition of mod ϕ\mathrm{mod}\, \phi.

Corollary

For all g∈Gg \in G, ΔG(g)=(mod⁡det⁡Ad⁡g)−1\Delta_G(g) = (\operatorname{mod} \det \operatorname{Ad} g)^{-1}. In particular, for GG to be unimodular, it is necessary and sufficient that mod⁡det⁡Ad⁡g=1\operatorname{mod} \det \operatorname{Ad} g = 1 for all g∈Gg \in G.

ΔG(g)=(mod⁡Int⁡g)−1(Integration, Chapter VII, § 1, formula (33))=(mod⁡det⁡L(Int⁡g))−1(Proposition 55)=(mod⁡det⁡Ad⁡g)−1. \Delta_G(g) = (\operatorname{mod} \operatorname{Int} g)^{-1} \quad \text{(Integration, Chapter VII, § 1, formula (33))} = (\operatorname{mod} \det L(\operatorname{Int} g))^{-1} \quad \text{(Proposition 55)} = (\operatorname{mod} \det \operatorname{Ad} g)^{-1}.

Remark

Preserving the hypotheses and notation of Proposition 52, suppose that KK is locally compact. Let μ\mu be the measure

mod⁡det⁡(Dn+imk(x1,…,xn,x1,…,xn))1≤i,k≤ndx1…dxn \operatorname{mod} \det(D_{n+i}m_k(x_1, \ldots, x_n, x_1, \ldots, x_n))_{1 \leq i, k \leq n} dx_1 \ldots dx_n
on ψ(U)\psi(U). Then ψ−1(μ)\psi^{-1}(\mu) is the restriction to UU of a Haar measure on GG.

Proposition 56

Let GG be a Lie group of finite dimension nn, HH a pp-dimensional Lie subgroup and XX the Lie homogeneous space G/HG/H. Suppose that

det⁡Ad⁡L(G)h=det⁡Ad⁡L(H)h \det \operatorname{Ad}_{L(G)} h = \det \operatorname{Ad}_{L(H)} h
for all h∈Hh \in H. Then: (i) The differential forms of degree n−pn - p on XX which are invariant under GG are analytic. (ii) The vector space of these forms is of dimension 1. (iii) If ω\omega is such a non-zero form and KK is locally compact, mod⁡(ω)μ\operatorname{mod}(\omega)_\mu is a non-zero measure on XX which is invariant under GG.

By § 1, no. 8, Examples, Alt⁡n−p(TX,K)\operatorname{Alt}^{n-p}(TX, K) is an analytic vector GG-bundle. Let x0x_0 be the canonical image of ee in XX; its stabilizer is HH. The fibre of Alt⁡n−p(TX,K)\operatorname{Alt}^{n-p}(TX, K) at x0x_0 is ⋀n−pTx0(X)∗\bigwedge^{n-p} T_{x_0}(X)^* and Tx0(X)T_{x_0}(X) is canonically identified with L(G)/L(H)L(G)/L(H). If h∈Hh \in H, the automorphism τh\tau_h of XX defined by hh is derived when passing to the quotient from the automorphism g↦hgh−1g \mapsto hgh^{-1} of GG. Hence the automorphism Tx0(τh)T_{x_0}(\tau_h) is derived when passing to the quotient from Ad⁡L(G)(h)\operatorname{Ad}_{L(G)}(h). As

det⁡Ad⁡L(G)h=(det⁡Ad⁡L(H)h)⋅(det⁡Tx0(τh)), \det \operatorname{Ad}_{L(G)} h = (\det \operatorname{Ad}_{L(H)} h) \cdot (\det T_{x_0}(\tau_h)),
the hypothesis implies that det⁡Tx0(h)=1\det T_{x_0}(h) = 1. Thus, every element of ⋀n−pTx0(X)∗\bigwedge^{n-p} T_{x_0}(X)^* is invariant under HH. Then (i) and (ii) follow from § 1, no. 8, Corollary 1 to Proposition 17 and (iii) is obvious.

The existence of a non-zero positive measure on XX invariant under GG follows from Integration, Chapter VII, § 2, Corollary 2 to Theorem 3, for the hypothesis of Proposition 56 implies ΔG∣H=ΔH\Delta_G|H = \Delta_H (Corollary to Proposition 55).

Proposition 57

Let GG be a Lie group of finite dimension nn. Choose a basis for ⋀nTe(G)∗\bigwedge^n T_e(G)^*; by means of the right (resp. left) trivialization of ⋀nT(G)∗\bigwedge^n T(G)^*, we can identify this vector bundle with the trivial vector bundle G×KG \times K, so that the transpose of a scalar differential operator is identified with a scalar differential operator.

Then, if u∈U(G)u \in U(G), the transpose of LuL_u (resp. RuR_u) is LuνL_u^\nu (resp. RuνR_u^\nu).

We shall consider the case where ΛnT(G)∗\Lambda^n T(G)^* has been trivialized using a right invariant form ω\omega.

Suppose that the proposition has been proved for elements u1,u2u_1, u_2 of U(G)U(G). Then,

t(Lu1∗u2)=t(Lu1∘Lu2)(Proposition 23)=t(Lu2)∘t(Lu1)(Diff. & Anal. Man., R, 14.3.3)=Lu2ν∘Lu1νby hypothesis=Lu2∗u1νν(Proposition 23)=L(u1∗u2)ν(Proposition 7) \begin{align*} t(L_{u_1 * u_2}) &= t(L_{u_1} \circ L_{u_2}) & \text{(Proposition 23)} \\ &= t(L_{u_2}) \circ t(L_{u_1}) & \text{(\emph{Diff. \& Anal. Man.}, R, 14.3.3)} \\ &= L_{u_2}^\nu \circ L_{u_1}^\nu & \text{by hypothesis} \\ &= L_{u_2 * u_1}^{\nu \nu} & \text{(Proposition 23)} \\ &= L_{(u_1 * u_2)^\nu} & \text{(Proposition 7)} \end{align*}

and hence the proposition is true for u1∗u2u_1 * u_2. It therefore suffices to prove the proposition when u∈Te(G)u \in T_e(G). Now LuL_u is defined by GG operating on GG on the right (no. 6) and hence θLuω=0\theta_{L_u} \omega = 0 since ω\omega is right invariant (\emph{Differentiable and Analytic Manifolds}, R, 8.4.5); therefore, if ff is an analytic function in an open neighbourhood of ee with values in KK, then θLu(fω)=(θLuf)ω\theta_{L_u}(f \omega) = (\theta_{L_u} f) \omega (\emph{Differentiable and Analytic Manifolds}, R, 8.4.8). Using the identifications made and \emph{Differentiable and Analytic Manifolds}, R, 14.4.1, the transpose of LuL_u is −Lu-L_u, that is LuνL_u^\nu.

Corollary

Let GG be a finite-dimensional real Lie group, μ\mu (resp. ν\nu) a left (resp. right) Haar measure on GG, kk an integer ⩾0\geqslant 0, u∈Uk(G)u \in U_k(G) and ff and gg real-valued functions of class CkC^k on GG with compact support. Then

∫G(Ruf)g dμ=∫Gf(Ruνg) dμ \int_G (R_u f) g \, d\mu = \int_G f (R_u^\nu g) \, d\mu
∫G(Luf)g dν=∫Gf(Luνg) dν. \int_G (L_u f) g \, d\nu = \int_G f (L_u^\nu g) \, d\nu.

This follows from Proposition 57 and \emph{Differentiable and Analytic Manifolds}, R, 14.3.8.

17. Left differential

Definition 9

Let GG be a Lie group, MM a manifold of class CrC^r and ff a mapping of class CrC^r of MM into GG. The left (resp. right) differential of ff is the differential form of degree 1 on MM with values in L(G)L(G) which associates with every vector u∈Tm(M)u \in T_m(M) the element f(m)−1⋅(Tmf)(u)f(m)^{-1} \cdot (T_m f)(u) (resp. (Tmf)(u)⋅f(m)−1(T_m f)(u) \cdot f(m)^{-1}).

In this chapter we shall only consider the left differential, which we shall denote by f−1.dff^{-1}.df, and leave to the reader the task of translating the results for the right differential.

If ff is the identity mapping of GG, f−1.dff^{-1}.df is the canonical left differential form ω\omega of GG. Returning to the general case of Definition 8,

(f−1.df)m=ωf(m)∘Tm(f) (f^{-1}.df)_m = \omega_{f(m)} \circ T_m(f)

and hence f−1.df=f∗(ω)f^{-1}.df = f^*(\omega). This implies that f−1.dff^{-1}.df is of class Cr−1C^{r-1}.

Example

(1) If GG is the additive group of a complete normable space and T0(E)T_0(E) is canonically identified with EE, f−1.dff^{-1}.df is the differential dfdf defined in Differentiable and Analytic Manifolds, R, 8.2.2.

(2) Suppose that GG is the multiplicative group A∗A^* associated with a complete normable algebra AA. Then ff can be considered as a mapping of MM into AA and hence the differential dfdf in the sense of Differentiable and Analytic Manifolds, R, 8.2.2 is defined and the product f−1dff^{-1}df in the sense of Differentiable and Analytic Manifolds, R, 8.3.2 is defined. Clearly the latter form is identical with the left differential of ff.

Proposition 58

Let GG and HH be two Lie groups, MM a manifold of class CrC^r, ff a mapping of class CrC^r of MM into GG and hh a morphism of GG into HH. Then

(h∘f)−1.d(h∘f)=L(h)∘(f−1.df)=(h−1.dh)∘T(f). (h \circ f)^{-1}.d(h \circ f) = L(h) \circ (f^{-1}.df) = (h^{-1}.dh) \circ T(f).

For all x∈Mx \in M and u∈Tx(M)u \in T_x(M),

(h∘f)−1.d(h∘f)(u)=((h∘f)(x))−1.T(h∘f)(u). (h \circ f)^{-1}.d(h \circ f)(u) = ((h \circ f)(x))^{-1}.T(h \circ f)(u).

The latter expression is equal, on the one hand, to

T(h)(f(x)−1.T(f)(u))(§2,Proposition 5) T(h)(f(x)^{-1}.T(f)(u)) \quad (§ 2, \text{Proposition 5})
=Te(h)((f−1.df)(u)) = T_e(h)((f^{-1}.df)(u))

and, on the other hand, to

h(f(x))−1T(h)(T(f)u) h(f(x))^{-1}T(h)(T(f)u)
=(h−1.dh)(T(f)u). = (h^{-1}.dh)(T(f)u).

Proposition 59

Let GG be a Lie group, MM a manifold of class CrC^r, ff and gg mappings of class CrC^r of MM into GG and pp the canonical surjection of TMTM onto MM.

(i) (fg)−1.d(fg)=(Ad∘g∘p)−1∘(f−1.df)+g−1.dg.(fg)^{-1}.d(fg) = (\mathrm{Ad} \circ g \circ p)^{-1} \circ (f^{-1}.df) + g^{-1}.dg.

(ii) Writing h(m)=f(m)−1h(m) = f(m)^{-1} for all m∈Mm \in M,

h−1.dh=−(Ad∘f∘p)∘(f−1.df). h^{-1}.dh = -(\mathrm{Ad} \circ f \circ p) \circ (f^{-1}.df).

Assertion (i) follows from § 2, no. 2, Proposition 7. Assertion (ii) follows from (i) by putting g=hg = h.

Corollary 1

Let s∈Gs \in G and sgsg be the mapping x↦sg(x)x \mapsto sg(x) of MM into GG. Then

(sg)−1.d(sg)=g−1.dg. (sg)^{-1}.d(sg) = g^{-1}.dg.

This follows from Proposition 59 (i) taking ff to be the constant mapping x↦sx \mapsto s of MM into GG.

Corollary 2

If the mappings ff and gg of MM into GG have the same left differential, the tangent mapping to fg−1fg^{-1} is everywhere zero. If further KK is of characteristic 0, then fg−1fg^{-1} is locally constant.

By Proposition 59,

(fg−1)−1⋅d(fg−1)=(Ad∘g∘p)∘(f−1.df)−(Ad∘g∘p)∘(g−1.dg). (fg^{-1})^{-1} \cdot d(fg^{-1}) = (\mathrm{Ad} \circ g \circ p) \circ (f^{-1}.df) - (\mathrm{Ad} \circ g \circ p) \circ (g^{-1}.dg).

If f−1.df=g−1.dgf^{-1}.df = g^{-1}.dg, then (fg−1)−1⋅d(fg−1)=0(fg^{-1})^{-1} \cdot d(fg^{-1}) = 0, that is Tx(fg−1)=0T_x(fg^{-1}) = 0 for all x∈Mx \in M. This proves the first assertion. The second follows from it by Differentiable and Analytic Manifolds, R, 5.5.3.

Proposition 60

Let GG be a Lie group, of finite dimension if KK is of characteristic > 0, MM a manifold of class CrC^r, ff a mapping of class CrC^r of MM into GG and α\alpha the left differential of ff. Then dα+[α]2=0d\alpha + [\alpha]^2 = 0.

Let ω\omega be the canonical left differential form of GG. Using Corollary 1 to Proposition 51, no. 14, we have

dα=d(f∗(ω))=f∗(dω)=f∗(−[ω]2)=−[f∗(ω)]2=−[α]2. d\alpha = d(f^*(\omega)) = f^*(d\omega) = f^*(-[\omega]^2) = -[f^*(\omega)]^2 = -[\alpha]^2.

18. Lie algebra of a Lie group germ

In this no. (G,e,θ,m)(G, e, \theta, m) denotes a Lie group germ. A large part of the results of the § are still true with the same proof. We shall review those which we shall find useful.

18.1. Let Ω\Omega be the set of definition of mm. Let (g,g′)∈Ω, t∈Te(∞)(G), t′∈Tg′(∞)(G)(g, g') \in \Omega,\ t \in T_e^{(\infty)}(G),\ t' \in T_{g'}^{(\infty)}(G). As in no. 1, the convolution product of tt and t′t', denoted by t∗t′t * t', is the image of t⊗t′t \otimes t' under mm. We write U(G)=Te(∞)(G), Us(G)=Te(s)(G), U+(G)=Te(∞)+(G), Us+(G)=Te(s)+(G)U(G) = T_e^{(\infty)}(G),\ U_s(G) = T_e^{(s)}(G),\ U^+(G) = T_e^{(\infty)+}(G),\ U_s^+(G) = T_e^{(s)+}(G). For t,t′t, t' in U(G)U(G), t∗t′t * t' is defined and belongs to U(G)U(G). With the convolution product, U(G)U(G) is an associative algebra with unit element εe\varepsilon_e, filtered by the Us(G)U_s(G). The canonical isomorphism iG,ei_{G,e} of gr U(G)U(G) onto TS(Te(G))TS(T_e(G)) is an algebra isomorphism.

18.2. Let G,HG, H be Lie group germs and ϕ:G→H\phi : G \to H a morphism. If t∈U(G)t \in U(G), the image U(ϕ)(t)U(\phi)(t) of tt under ϕ∗\phi_* is an element of U(H)U(H) and U(ϕ)U(\phi) is a morphism of the algebra U(G)U(G) into the algebra U(H)U(H). The mapping θ:x↦x−1\theta : x \mapsto x^{-1} of GG into GG defines a mapping t↦t∨t \mapsto t^\vee of U(G)U(G) into U(G)U(G). For t,t′t, t' in U(G)U(G), the product t∗t′t * t' evaluated relative to G∨G^\vee is equal to the product t′∗tt' * t evaluated relative to GG and (t∗t′)∨=t′∨∗t∨(t * t')^\vee = {t'}^\vee * t^\vee. Then U(ϕ)(t∨)=(U(ϕ)t)∨U(\phi)(t^\vee) = (U(\phi)t)^\vee. If G1,…,GnG_1, \ldots, G_n are Lie group germs and G=G1×⋯×GnG = G_1 \times \cdots \times G_n, the canonical isomorphism of U(G1)⊗⋯⊗U(Gn)U(G_1) \otimes \cdots \otimes U(G_n) onto U(G)U(G) is an algebra isomorphism;

for t1,…,tnt_1, \ldots, t_n in U(G)U(G), (t1⊗⋯⊗tn)∨=t1∨⊗⋯⊗tn∨(t_1 \otimes \cdots \otimes t_n)^{\vee} = t_1^{\vee} \otimes \cdots \otimes t_n^{\vee}. Let HH be a Lie subgroup germ of GG and i:H→Gi : H \to G the canonical injection. Then U(i)U(i) is an injective homomorphism of the algebra U(H)U(H) into U(G)U(G) and

U(i)(t∨)=(U(i)(t))∨ U(i)(t^{\vee}) = (U(i)(t))^{\vee}
for all t∈U(H)t \in U(H). With the convolution product and the coproduct defined by the manifold structure on GG, U(G)U(G) is a bigebra and U(ϕ)U(\phi) is a bigebra morphism.

18.3. Let GG be a Lie group germ, XX a manifold of class CrC^r and ψ\psi a law chunk of left operation of class CrC^r of GG on XX. Let Ω\Omega be the set of definition of ψ\psi. If t∈Tg(s)(G)t \in T^{(s)}_g(G), u∈Tx(s′)(X)u \in T^{(s')}_x(X), (g,x)∈Ω(g, x) \in \Omega and s+s′≤rs + s' \leq r, let t∗ut * u denote the image of t⊗ut \otimes u under ψ∗\psi_*. Let t∈Tg(s)(G)t \in T^{(s)}_g(G), t′∈Tx(s′)(G)t' \in T^{(s')}_x(G), u∈Tx(s′′)(X)u \in T^{(s'')}_x(X); if s+s′+s′′≤rs + s' + s'' \leq r and gg′gg', (gg′)x(gg')x, g′xg'x, g(g′x)g(g'x) are defined, then

(t∗t′)∗u=t∗(t′∗u). (t * t') * u = t * (t' * u).
Let x0∈Xx_0 \in X and ρ(x0)\rho(x_0) be the mapping g↦gx0g \mapsto gx_0, which is defined in an open neighbourhood of ee. If t∈Ur(G)t \in U_r(G), then ρ(x0)∗t=t∗εx0\rho(x_0)_*t = t * \varepsilon_{x_0}. Here and in the rest of this no., we shall leave to the reader the task of translating the results for law chunks of right operation.

18.4. Preserving the notation of 18.3, let t∈Us(G)t \in U_s(G) with s≤rs \leq r. Let ff be a function of class CrC^r on XX with values in a Hausdorff polynormed space. Let t∗ft * f denote the function on XX defined by

(t∗f)(x)=⟨t,g↦f(ψ(θ(g),x))⟩=⟨t∨,f∘ρ(x)⟩=⟨ρ(x)∗(t∨),f⟩=⟨t∨∗εx,f⟩. \begin{align*} (t * f)(x) &= \langle t, g \mapsto f(\psi(\theta(g), x)) \rangle \\ &= \langle t^{\vee}, f \circ \rho(x) \rangle = \langle \rho(x)_*(t^{\vee}), f \rangle = \langle t^{\vee} * \varepsilon_x, f \rangle. \end{align*}
If t∈Us(G)t \in U_s(G), t′∈Us′(G)t' \in U_{s'}(G) and s+s′≤rs + s' \leq r, then ⟨t′,t∗f⟩=⟨t∨∗t′,f⟩\langle t', t * f \rangle = \langle t^{\vee} * t', f \rangle and (t∗t′)∗f=t∗(t′∗f)(t * t') * f = t * (t' * f). Let t∈Us(G)t \in U_s(G), ff and f′f' be functions of class CrC^r on XX with values in Hausdorff polynormed spaces F,F′F, F' and (u,u′)↦u.u′(u, u') \mapsto u.u' be a continuous bilinear mapping of F×F′F \times F' into a Hausdorff polynormed space; let
∑i=1nti⊗ti′ \sum_{i=1}^n t_i \otimes t'_i
be the image of tt under the coproduct; if s≤rs \leq r, then
t∗(ff′)=∑i=1n(ti∗f)(ti′∗f′). t * (ff') = \sum_{i=1}^n (t_i * f)(t'_i * f').

18.5. Preserving the notation of 18.3, let t∈Us(G)t \in U_s(G) with s≤rs \leq r. The mapping x↦t∗εxx \mapsto t * \varepsilon_x is called the field of point distributions defined by tt and the law chunk of operation and is sometimes denoted by DtψD_t^{\psi} or DtD_t. If f:X→Ff : X \to F is a function of class CrC^r, the function t∨∗ft^{\vee} * f on XX is also denoted by DtfD_t f; it is of class Cr−sC^{r-s} if s<∞s < \infty. If t∈Us(G)t \in U_s(G), t′∈Us′(G)t' \in U_{s'}(G) and s+s′≤rs + s' \leq r, then Dt∗t′f=Dt′(Dtf)D_{t*t'} f = D_{t'}(D_t f). If GG and XX are finite-dimensional, DtD_t is a differential operator on XX of order ≤s\leq s and of class Cr−sC^{r-s} (if s<∞s < \infty). The function DtfD_t f is then the transform of ff under this differential operator.

18.6. Let G be a Lie group germ and t∈U(G)t \in U(G). LtL_t denotes the field of point distributions g↦εg∗tg \mapsto \varepsilon_g * t on G and RtR_t the field of point distributions g↦t∗εgg \mapsto t * \varepsilon_g on G. If f∈Cω(G,F)f \in C^\omega(G, F), then Ltf∈Cω(G,F)L_t f \in C^\omega(G, F) and Rtf∈Cω(G,F)R_t f \in C^\omega(G, F). For t,t′t, t' in U(G)U(G), Lt∘t′=Lt∘Lt′L_{t \circ t'} = L_t \circ L_{t'}, Rt∘t′=Rt′∘RtR_{t \circ t'} = R_{t'} \circ R_t, Lt∘Rt′=Rt′∘LtL_t \circ R_{t'} = R_{t'} \circ L_t, θ(Lt)=RtV\theta(L_t) = R_t^V.

18.7. As Te(G)T_e(G) is the set of primitive elements of U(G)U(G),

[Te(G),Te(G)]⊂Te(G). [T_e(G), T_e(G)] \subset T_e(G).

The normable space Te(G)T_e(G), together with the bracket, is a normable Lie algebra, called the normable Lie algebra of G (or Lie algebra of G) and denoted by L(G)L(G). Let E(G)E(G) be the enveloping algebra of L(G)L(G). The canonical injection of L(G)L(G) into U(G)U(G) defines a homomorphism η\eta of the algebra E(G)E(G) into the algebra U(G)U(G); if K is of characteristic 0, η\eta is a bigebra isomorphism, by means of which U(G)U(G) is identified with E(G)E(G). Using the notation of 18.3, for all a∈L(G)a \in L(G), let DaD_a be the field of point distributions defined by aa on X. The mapping (a,x)↦Da(x)(a, x) \mapsto D_a(x) is a morphism of class Cr−1C^{r-1} of the trivial vector bundle L(G)×XL(G) \times X into the vector bundle T(X)T(X). Let I be an open subset of K containing 0 and γ:I→G\gamma : I \to G a mapping of class CrC^r such that γ(0)=e\gamma(0) = e. Let a=T0(γ)l∈L(G)a = T_0(\gamma) l \in L(G). If f:X→Ff : X \to F is a function of class CrC^r, then

(Daf)(x)=lim⁡k∈K∗,k→0k−1(f(γ(k)x)−f(x)). (D_a f)(x) = \lim_{k \in K^*, k \to 0} k^{-1}(f(\gamma(k)x) - f(x)).

If r≥2r \geq 2, the mapping a↦Daa \mapsto D_a is a law of left infinitesimal operation of class Cr−1C^{r-1} of L(G)L(G) on X.

18.8. Let G and H be Lie group germs and ϕ\phi a morphism of G into H. The restriction of U(ϕ)U(\phi) to L(G)L(G), which is just Te(ϕ)T_e(\phi), is a continuous morphism of L(G)L(G) into L(H)L(H), which we denote by L(ϕ)L(\phi). If ψ\psi is a morphism of H into a Lie group germ, then L(ψ∘ϕ)=L(ψ)∘L(ϕ)L(\psi \circ \phi) = L(\psi) \circ L(\phi). For ϕ\phi to be an immersion, it is necessary and sufficient that L(ϕ)L(\phi) be an isomorphism of L(G)L(G) onto a Lie subalgebra of L(H)L(H) which admits a topological supplement. In particular, if G is a Lie subgroup germ of H and ϕ\phi is the canonical injection, L(G)L(G) is identified with a Lie subalgebra of L(H)L(H) by means of L(ϕ)L(\phi). If (Gi)i∈I(G_i)_{i \in I} is a finite family of Lie group germs and G is their product, L(G)L(G) is canonically identified with ∏i∈IL(Gi)\prod_{i \in I} L(G_i).

18.9. Let G be a Lie group germ, of finite dimension if K is of characteristic > 0. Let F be a complete normable space. Let α\alpha be a differential form of degree k on G with values in F. α\alpha is called left invariant on G if αg\alpha_g is derived from αe\alpha_e by the mapping h↦ghh \mapsto gh of a neighbourhood of e onto a neighbourhood of g. If α\alpha is left invariant, α\alpha is analytic. The mapping α↦αe\alpha \mapsto \alpha_e is a bijection of the set of left invariant differential forms of degree k on G with values in F onto the set of continuous alternating k-linear mappings of Te(G)T_e(G) into F. If αe=IdTe(G)\alpha_e = \mathrm{Id}_{T_e(G)}, α\alpha is called the left canonical differential form of G. The definitions of right invariant differential forms and the right canonical differential form of G are analogous. If ω\omega is the left canonical differential form of G, then dω+[ω]2=0d\omega + [\omega]^2 = 0. Let M be a manifold of class CrC^r and ff a mapping of class CrC^r of M into G. The left differential of ff, denoted by f−1.dff^{-1}.df, is the differential form of degree 1 on M with values in L(G)L(G) which associates with each vector u∈Tm(M)u \in T_m(M) the element f(m)−1.(Tm,f)(u)f(m)^{-1}.(T_{m,f})(u). Then f−1.df=f∗(ω)f^{-1}.df = f^*(\omega) and dα+[α]2=0d\alpha + [\alpha]^2 = 0. If two mappings ff and gg of M into G have the same left differential and K is of characteristic 0, then fg−1fg^{-1} is locally constant.

Exercises

See the exercises for § 3.

Transcribed from the printed volume. Not translated.