Bourbaki

§ 8. The differential calculus of order 1

Starting from No. 8.3, we suppose

— either that KK is of characteristic zero,

— or that the varieties under consideration are locally of finite dimension.

In the latter case, the expressions “Banach space, vector bundle, vector functor” mean respectively “finite-dimensional vector space, vector bundle of finite rank, vector functor in finite dimension with values of finite dimension”.

8.1. Tangent bundle

8.1.1. — Let r∈NKr\in \mathbf{N}_K and let XX be a KK-variety of class CrC^r. We denote by T(X)T(X) the sum set of the tangent spaces Tx(X)T_x(X) (5.5.1) for x∈Xx\in X, and by π\pi the canonical mapping of T(X)T(X) onto XX. Let c=(U,φ,E)c=(U,\varphi,E) be a chart of the variety XX; for x∈Ux\in U and t∈Tx(X)t\in T_x(X), put ζc(x,t)=(x,θc−1(t))\zeta_c(x,t)=(x,\theta_c^{-1}(t)), the mapping θc\theta_c being that defined in 5.5.1. The triplet c′=(U,ζc,E)c'=(U,\zeta_c,E) is a vector chart (7.1.1) of T(X)T(X) (endowed with the mapping π:T(X)⟶X\pi:T(X)\longrightarrow X). There exists on T(X)T(X) one and only one structure of vector bundle with base XX and of class Cr−1C^{r-1} such that, for every chart cc of XX, the corresponding vector chart c′c' is a vector chart of T(X)T(X)[^1]. Endowed with this structure, T(X)T(X) is called the tangent bundle of XX. In particular, T(X)T(X) is endowed with a structure of variety of class Cr−1C^{r-1} and the triplet (T(X),X,π)(T(X),X,\pi) is a fibration (7.1.4).

Let UU be an open subset of a Banach space EE and let ii be the canonical injection of UU into EE. The vector chart c′=(U,ζc,E)c'=(U,\zeta_c,E) associated with the chart c=(U,i,E)c=(U,i,E) of UU defines an isomorphism of T(U)T(U) onto the trivial bundle EUE_U (7.1.5); these two bundles are identified by means of this isomorphism.

If XX is a purely variety of type EE (5.1.7), T(X)T(X) is a purely variety of type E×EE\times E.

8.1.2. — Let f:X⟶Yf:X\longrightarrow Y be a morphism of varieties of class CrC^r. We define an ff-morphism T(f):T(X)⟶T(Y)T(f):T(X)\longrightarrow T(Y) of vector bundles of class Cr−1C^{r-1} by

T(f)(x,t)=(f(x),Txf(t)) T(f)(x,t)=(f(x),T_xf(t))
for x∈Xx\in X and t∈Tx(X)t\in T_x(X).

If f=IdXf=\mathrm{Id}_X, one has T(f)=IdT(X)T(f)=\mathrm{Id}_{T(X)}. For f:X⟶Yf:X\longrightarrow Y and g:Y⟶Zg:Y\longrightarrow Z, one has

T(g∘f)=T(g)∘T(f). T(g\circ f)=T(g)\circ T(f).

8.1.3. — Let f:X⟶Yf:X\longrightarrow Y be a morphism of manifolds of class CrC^r, and let f′:T(X)⟶f∗T(Y)f':T(X)\longrightarrow f^*T(Y)

be the unique X-morphism such that T(f) = g ∘ f', where g is the canonical morphism f*T(Y) → T(Y) (cf. 7.2.4).

For f to be an immersion (resp. a submersion), it is necessary and sufficient that 0 → T(X) →f′f∗T(Y)\xrightarrow{f'} f^*T(Y) (resp. T(X) →f′f∗T(Y)→0\xrightarrow{f'} f^*T(Y) \to 0) be a locally direct exact sequence (7.5.6). If f is an immersion, the cokernel bundle of f' is called the normal or transverse bundle of f. If f is a submersion, the kernel bundle of f is called the tangent bundle to the fibres of f, or the relative tangent bundle of X over Y, and is denoted T(X/Y). Its fibre T_x(X/Y) at x ∈ X is the tangent space at x to the submanifold f−1(f(x))f^{-1}(f(x)) of X. The sequence

0⟶Tx(X/Y)→iTx(X)→Tx(f)Tf(x)(Y)⟶0 0 \longrightarrow T_x(X/Y) \xrightarrow{i} T_x(X) \xrightarrow{T_{x(f)}} T_{f(x)}(Y) \longrightarrow 0

where i is the canonical injection, is exact.

For f to be étale, it is necessary and sufficient that f' be an isomorphism.

When K has characteristic 0, for f to be a subimmersion, it is necessary and sufficient that f' be locally direct.

8.1.4. Let X_1 and X_2 be two manifolds. We have T(X_1 × X_2) = p_1^*T(X_1) ⊕ p_2^*T(X_2), where p_1 and p_2 are the canonical projections (5.6.3).

8.1.5. Let n be an integer ⩾0\geqslant 0; the tangent bundle T(K^n) of K^n is identified with the trivial bundle with fibre K^n (8.1.1). The constant sections defined by the elements of the canonical basis of K^n form a frame of T(K^n).

If X is a manifold and (u^1, ..., u^n) a system of coordinates of X in an open set U of X (5.1.10), the preceding frame defines by transport of structure a frame of T(X) on U; it is called the tangent frame defined by (u^1, ..., u^n) and is denoted (\partial/\partial u^1, ..., \partial/\partial u^n) (cf. 5.5.8).

8.2. Vector fields

Let X be a manifold of class C^r, and let U be an open set of X.

8.2.1. A section (not necessarily continuous, cf. Notations and Conventions) of the tangent bundle T(X) above U is called a vector field on U.

8.2.2. The dual bundle T'(X) (7.7.3) of T(X) is called the cotangent bundle of X. Its sections are called covector fields. If f is a function of class C^k on X (with 1 ≤ k ≤ r), with values in K, its differential df : x ↦ d_x f (5.5.6) is a covector field of class C^{k-1}. More generally, if f is a function of class C^k on X (1 ≤ k ≤ r), with values in a Banach space E, its differential df is a section of class C^{k-1} of the bundle L(T(X);EX)\mathscr{L}(T(X); E_X).

8.2.3. Let ξ\xi be a vector field of class C^{r-1} on X, and let f∈Cr(X;F)f \in \mathscr{C}^r(X; F) be a function of class C^r with values in a Banach space F. We denote by ⟨ξ,df⟩\langle \xi, df \rangle, or D_\xi(f), or again ξ(f)\xi(f) the function x↦dxf(ξ(x))x \mapsto d_x f(\xi(x)); it is an element of Cr−1(X;F)\mathscr{C}^{r-1}(X; F). For fixed f, the mapping ξ↦Dξ(f)\xi \mapsto D_\xi(f) is Cr−1(X)\mathscr{C}^{r-1}(X)-linear. If Dξf=0D_\xi f = 0 for every function f of class C^r with values in a Banach space, defined in an open set of X, we have ξ=0\xi = 0.

Let E, F, G be Banach spaces and let (u, v) ↦ u . v be a continuous bilinear mapping of E×FE \times F into GG. Let f∈Cr(X;E)f \in \mathscr{C}^r(X; E), g∈Cr(X;F)g \in \mathscr{C}^r(X; F) and let f.g∈Cr(X;G)f.g \in \mathscr{C}^r(X; G) be their product. If ξ\xi is a vector field of class Cr−1C^{r-1} on XX, we have

Dξ(f.g)=Dξ(f).g+f.Dξ(g). D_\xi(f.g) = D_\xi(f).g + f.D_\xi(g).
In particular, the mapping Dξ:Cr(X)→Cr−1(X)D_\xi : \mathscr{C}^r(X) \to \mathscr{C}^{r-1}(X) is a derivation of the algebra Cr(X)\mathscr{C}^r(X) into the Cr(X)\mathscr{C}^r(X)-module Cr−1(X)\mathscr{C}^{r-1}(X).

8.2.4. Suppose that XX is locally of finite dimension and that one of the following two hypotheses is satisfied:

(i) r=∞r = \infty and XX is separated; (ii) r=ωr = \omega and XX is isomorphic to an open polydisc of KnK^n.

Then, for every derivation DD of the algebra Cr(X)\mathscr{C}^r(X), there exists one and only one vector field ξ\xi of class CrC^r such that D=DξD = D_\xi.

8.2.5. Let (u1,…,un)(u^1, \ldots, u^n) be a system of coordinates of XX in UU, and ξ\xi a vector field on UU. The ii-th coordinate of ξ\xi in the tangent frame (8.1.5) defined by (u1,…,un)(u^1, \ldots, u^n) is Dξ(ui)D_\xi(u^i). In other words, we have

ξ=∑1≤i≤nDξ(ui)⋅∂/∂ui. \xi = \sum_{1 \leq i \leq n} D_\xi(u^i) \cdot \partial/\partial u^i.

8.2.6. Let φ:X→Y\varphi : X \to Y be a morphism of manifolds of class CrC^r, ξ\xi a vector field on XX and η\eta a vector field on YY. We say that ξ\xi is φ\varphi-*related* to η\eta if, for every x∈Xx \in X, we have η(φ(x))=Tx(φ)(ξ(x))\eta(\varphi(x)) = T_x(\varphi)(\xi(x)). Suppose this is so, and that ξ\xi and η\eta are of class Cr−1C^{r-1}. Then, for every Banach space EE, the diagram

Cr(Y;E)→φ∗Cr(X;E)↓Dη↓DξCr−1(Y;E)→φ∗Cr−1(X;E) \begin{array}{ccc} \mathscr{C}^r(Y; E) & \xrightarrow{\varphi^*} & \mathscr{C}^r(X; E) \\ \downarrow D_\eta & & \downarrow D_\xi \\ \mathscr{C}^{r-1}(Y; E) & \xrightarrow{\varphi^*} & \mathscr{C}^{r-1}(X; E) \end{array}

where φ∗(f)=f∘φ\varphi^*(f) = f \circ \varphi, is commutative.

When φ\varphi is étale, for every vector field η\eta on YY, there exists one and only one vector field on XX which is φ\varphi-*related* to η\eta; it is denoted by φ∗η\varphi^*\eta.

8.2.7. Let φ:X→Y\varphi : X \to Y be a morphism of manifolds of class CrC^r. If ω\omega is a covector field(1)^{(1)} on YY, we define a covector field φ∗ω\varphi^*\omega on XX by

(φ∗ω)(x)=t(Tx(φ))(ω(φ(x)))(x∈X). (\varphi^*\omega)(x) = t(T_x(\varphi))(\omega(\varphi(x))) \quad (x \in X).
More generally, let τ\tau be a vector functor (7.6) of class Cr−1C^{r-1}, of type (I+,I−)(I_+, I_-) with I+=∅I_+ = \emptyset and I−I_- reduced to one element (such a functor is said to be contravariant). If ω\omega is a section of class Cr−1C^{r-1} of the vector bundle τ(T(Y))\tau(T(Y)) based on YY, we define a section φ∗ω\varphi^*\omega of τ(T(X))\tau(T(X)) by (φ∗ω)(x)=τ(Tx(φ))(ω(φ(x)))(\varphi^*\omega)(x) = \tau(T_x(\varphi))(\omega(\varphi(x))) (x∈X)(x \in X).

1^1 The reader should take care not to confuse this use of the letter ω\omega with that defined in Notations and Conventions.

8.3. Differential forms, exterior differentiation

Let us recall that, in this number and the following ones, it is assumed either that K is of characteristic 0, or that the manifolds considered are locally of finite dimension.

8.3.1. Let X be a manifold of class C' and F a vector bundle of class C^k based on X, with k + 1 \in \mathbf{N}_K and k + 1 \leq r. Let p be an integer ≥0\geq 0 and let Alt^p(T(X); F) be the vector bundle of class C^k of alternating p-linear mappings of T(X) into F (7.8.1 and Errata to No. 7.8). A section of this bundle over an open set U of X is called an alternating differential form (or simply differential form) of degree p on U, with values in F. Those of these sections which are of class C^k form a Ck(U)\mathscr{C}^k(U)-module, denoted ^k\Omega^p(U; F). If E is a Banach space, we write ^k\Omega^p(U; E) instead of ^k\Omega^p(U; E_X) and speak of differential forms with values in E. In this notation, k (resp. E) is sometimes omitted when it is equal to r − 1 (resp. K).

A differential form of degree 0 (resp. 1) with scalar values is a function (resp. a covector field).

Let φ:Y→X\varphi : Y \to X be a morphism of manifolds of class C', and let ω∈kΩp(X;F).Therethenexistsoneandonlyoneform\omega \in ^k\Omega^p(X; F). There then exists one and only one form \varphi^*\omega \in ^k\Omega^p(Y; \varphi^*F) such that

(1)

(φ∗ω)y(v1,…,vp)=ωφ(y)(Ty(φ).v1,…,Ty(φ).vp)(\varphi^*\omega)_y(v_1, \ldots, v_p) = \omega_{\varphi(y)}(T_y(\varphi).v_1, \ldots, T_y(\varphi).v_p)

for every y \in Y and every family v_1, \ldots, v_p of elements of T_y(Y).

If ψ:Z→Y\psi : Z \to Y is a morphism of manifolds of class C', we have

(2)

(φ∘ψ)∗ω=ψ∗(φ∗ω).(\varphi \circ \psi)^*\omega = \psi^*(\varphi^*\omega).

When Y is a submanifold of X and φ\varphi is the canonical injection, we sometimes write ω∣Y\omega|Y instead of φ∗ω\varphi^*\omega and say that ω∣Y\omega|Y is induced on Y by ω\omega.

8.3.2. The definitions and results of No. 7.8 apply to differential forms. In particular, a pairing of vector bundles F' \times_X F'' \to F gives rise to an exterior product ^k\Omega^{p'}(U; F) \times ^k\Omega^{p''}(U; F'') \to ^k\Omega^p(U; F), where p = p' + p'' (7.8.2); it is denoted by (ω′,ω′′)↦ω′∧ω′′(\omega', \omega'') \mapsto \omega' \wedge \omega''. The direct sum of the ^k\Omega^p(U; K) for p \geq 0 is thus endowed with a structure of associative and alternating graded algebra (A, III, p. 53).

Let ξ\xi be a vector field on X and ω\omega a differential form of degree p \geq 1 on X, with values in a vector bundle F; the interior product of ξ\xi and ω\omega is the differential form i(\xi, \omega) of degree p − 1 on X, with values in F, defined by

(3)

i(ξ,ω)x(v1,…,vp−1)=ωx(ξ(x),v1,…,vp−1)i(\xi, \omega)_x(v_1, \ldots, v_{p-1}) = \omega_x(\xi(x), v_1, \ldots, v_{p-1})

for every x \in X and every family v_1, \ldots, v_{p-1} of elements of T_x(X). If ω\omega is a differential form of degree 0, we put i(\xi, \omega) = 0. We also write i(\xi)\omega or i_\xi\omega instead of i(\xi, \omega). When F = K_X, the definition given above coincides with that of 7.8.4.

Let F' \times_X F'' \to F be a pairing of vector bundles. For ω′∈kΩp′(U;F′)and\omega' \in ^k\Omega^{p'}(U; F') and \omega'' \in ^k\Omega^{p''}(U; F''), we have

(4)

i(ξ)(ω′∧ω′′)=(i(ξ)ω′)∧ω′′+(−1)p′ω′∧i(ξ)ω′′.i(\xi)(\omega' \wedge \omega'') = (i(\xi)\omega') \wedge \omega'' + (-1)^{p'\omega'} \wedge i(\xi)\omega''.

8.3.3. Let (u1,…,un)(u^1, \ldots, u^n) be a system of coordinates in the open set UU of XX. Every element ω\omega of kΩp(U;F)^{k}\Omega^p(U; F) is written in a unique way

ω=∑i1<⋯<ipfi1,…,ip⋅dui1∧⋯∧duip \omega = \sum_{i_1 < \cdots < i_p} f_{i_1, \ldots, i_p} \cdot du^{i_1} \wedge \cdots \wedge du^{i_p}
where the fi1,…,ipf_{i_1, \ldots, i_p} are sections of class CkC^k of FF on UU; in this formula, the sign ∧\wedge is relative to the canonical pairing KX×XKX→KXK_X \times_X K_X \to K_X and the point designating the product is relative to the canonical pairing F×XKX→FF \times_X K_X \to F.

8.3.4. Let pp be an integer ⩾0\geqslant 0 and rr an element of NKN_K. Let EE and FF be Banach spaces, UU an open set of EE and α∈rΩp(U;F)\alpha \in {}^r\Omega^p(U; F). Let α~∈Cr(U;Altp(E;F))\tilde{\alpha} \in C^r(U; Alt^p(E; F)) be the element corresponding to α\alpha. If x∈Ux \in U, the differential dxα~d_x \tilde{\alpha} of α~\tilde{\alpha} at xx (5.5.6) is an element of L(E;Altp(E;F))\mathscr{L}(E; Alt^p(E; F)); if t∈Et \in E, we have (dxα~)(t)∈Altp(E;F)(d_x \tilde{\alpha})(t) \in Alt^p(E; F), and, if t1,…,tpt_1, \ldots, t_p are in EE, we have (dxα~)(t)(t1,…,tp)∈F(d_x \tilde{\alpha})(t)(t_1, \ldots, t_p) \in F. There exists one and only one element dαd\alpha of r−1Ωp+1(U;F){}^{r-1}\Omega^{p+1}(U; F) such that one has

(dα)x(t0,…,tp)=∑i=0p(−1)i(dxα~)(ti)(t0,…,t^i,…,tp)(1) (d\alpha)_x(t_0, \ldots, t_p) = \sum_{i=0}^p (-1)^i (d_x \tilde{\alpha})(t_i)(t_0, \ldots, \hat{t}_i, \ldots, t_p) \tag{1}
whatever x∈Ux \in U and t0,…,tpt_0, \ldots, t_p in EE may be.

8.3.5. Let pp be an integer ⩾0\geqslant 0 and rr an element of NKN_K. Let XX be a variety of class Cr+1C^{r+1}, FF a Banach space, and ω∈rΩp(X;F)\omega \in {}^r\Omega^p(X; F). There exists one and only one differential form π∈r−1Ωp+1(X;F)\pi \in {}^{r-1}\Omega^{p+1}(X; F) such that, for every chart c=(U,φ,E)c = (U, \varphi, E) of XX, if ωc\omega_c is the differential form on φ(U)\varphi(U) such that ω∣U=φ∗(ωc)\omega|U = \varphi^*(\omega_c), one has πc=dωc\pi_c = d\omega_c, where dωcd\omega_c is defined by formula (5) of 8.3.4.

The differential form π\pi is called the exterior differential of ω\omega; it is denoted dωd\omega. It has the following properties:

(6) If ψ:Y→X\psi : Y \to X is a morphism of manifolds of class Cr+1C^{r+1}, and if ω∈rΩp(X;F)\omega \in {}^r\Omega^p(X; F), one has ψ∗(dω)=d(ψ∗ω)\psi^*(d\omega) = d(\psi^*\omega); in particular, dd commutes with the operation of restriction to a submanifold. (7) For p=0p = 0, the mapping d:rΩ0(X;F)→r−1Ω1(X;F)d : {}^r\Omega^0(X; F) \to {}^{r-1}\Omega^1(X; F) coincides with that defined in 8.2.2. (8) If r⩾2r \geqslant 2 and if ω∈rΩp(X;F)\omega \in {}^r\Omega^p(X; F), one has d(dω)=0d(d\omega) = 0.\footnote{The sign ∧\wedge indicates that the symbol above which it is placed is to be omitted (cf. 7.8.4).} (9) For every continuous linear mapping u:F→F′u : F \to F' of Banach spaces, one has d(u(ω))=u(d(ω))d(u(\omega)) = u(d(\omega)) for ω∈rΩp(U;F)\omega \in {}^r\Omega^p(U; F). (10) For every continuous bilinear mapping F′×F′′→FF' \times F'' \to F of Banach spaces, one has

d(ω′∧ω′′)=(dω′)∧ω′′+(−1)p′ω′∧dω′′ d(\omega' \wedge \omega'') = (d\omega') \wedge \omega'' + (-1)^{p'} \omega' \wedge d\omega''
for ω′∈rΩp′(X;F′)\omega' \in {}^r\Omega^{p'}(X; F') and ω′′∈rΩp′′(X;F′′)\omega'' \in {}^r\Omega^{p''}(X; F'').

8.3.6. Let (u1,…,un)(u^1, \ldots, u^n) be a system of coordinates of XX in UU. Let

ω=∑i1<⋯<ipfi1,…,ip⋅dui1∧⋯∧duip \omega = \sum_{i_1 < \cdots < i_p} f_{i_1, \ldots, i_p} \cdot du^{i_1} \wedge \cdots \wedge du^{i_p}

1 The sign ∧\wedge indicates that the symbol above which it is placed is to be omitted (cf. 7.8.4). 2 If ω∈1Ωp(X;F)\omega \in {}^1\Omega^p(X; F) and if dω∈1Ωp+1(X;F)d\omega \in {}^1\Omega^{p+1}(X; F), one still has d(dω)=0d(d\omega) = 0.

a differential form on U (with fi1,...,ip∈Cr(U;F)f_{i_1, ..., i_p} \in \mathscr{C}^r(U; F)). One then has

dω=∑i1<...<ipdfi1,...,ip∧dui1∧⋯∧duip. d\omega = \sum_{i_1 < ... < i_p} df_{i_1, ..., i_p} \wedge du^{i_1} \wedge \cdots \wedge du^{i_p}.

8.3.7. Suppose that K is of characteristic zero. Let ω∈rΩp(X;F)\omega \in {}^r\Omega^p(X; F) be a differential form of degree p≥1p \geq 1 such that dω=0d\omega = 0. For every x∈Xx \in X, there exists an open neighbourhood U of xx and a differential form π∈rΩp−1(U;F)\pi \in {}^r\Omega^{p-1}(U; F) such that dπ=ωd\pi = \omega on U.

8.4. Infinitesimal transformations

Let r∈NKr \in \mathbf{N}_K and X be a manifold of class Cr+1C^{r+1}.

8.4. Infinitesimal transformations

8.4.1. Let τ\tau be a vector functor for isomorphisms (7.6.6), of class CrC^r. If E is a Banach space, denote by GL(E)\mathbf{GL}(E) the open subset of L(E;E)\mathscr{L}(E; E) consisting of the automorphisms of E. Denote by τE′\tau'_E the tangent linear mapping at the identity element IdE\mathrm{Id}_E of the morphism τ:GL(E)→GL(τ(E))\tau : \mathbf{GL}(E) \to \mathbf{GL}(\tau(E)); it is a continuous linear mapping of L(E;E)\mathscr{L}(E; E) into L(τ(E);τ(E))\mathscr{L}(\tau(E); \tau(E)).

8.4.2. Let E be a Banach space and put F=τ(E)F = \tau(E). Let U be an open subset of E, ξ\xi a vector field on U of class CrC^r, ξ~:U→E\tilde{\xi} : U \to E the corresponding mapping (obtained by identifying T(U) and U×EU \times E (8.1.1)), and f:U→Ff : U \to F a mapping of class CrC^r. For x∈Ux \in U, define an element (θξ.f)(x)(\theta_{\xi}.f)(x) of F by the formula

(θξ.f)(x)=dxf(ξ~(x))−τE′(dxξ~)(f(x)). (\theta_{\xi}.f)(x) = d_x f(\tilde{\xi}(x)) - \tau'_E(d_x \tilde{\xi})(f(x)).

(Let us remark that on the one hand ξ~(x)∈E\tilde{\xi}(x) \in E and dxf∈L(E;F)d_x f \in \mathscr{L}(E; F), whence dxf(ξ~(x))∈Fd_x f(\tilde{\xi}(x)) \in F, and on the other hand, dxξ~∈L(E;E)d_x \tilde{\xi} \in \mathscr{L}(E; E), τE′(dxξ~)∈L(F;F)\tau'_E(d_x \tilde{\xi}) \in \mathscr{L}(F; F) and f(x)∈Ff(x) \in F, whence τE′(dxξ~)(f(x))∈F\tau'_E(d_x \tilde{\xi})(f(x)) \in F. The function θξ.f:x↦(θξ.f)(x)\theta_{\xi}.f : x \mapsto (\theta_{\xi}.f)(x) is of class Cr−1C^{r-1} in U.

8.4.3. Let F denote the vector bundle τ(T(X))\tau(T(X)) (7.6.2 and 7.6.6). Let ξ\xi be a vector field on X and ff a section of F, both of class CrC^r. Let xx be a point of X and c=(U,φ,E)c = (U, \varphi, E) a chart of X at xx. Let c′=(U,ζc,E)c' = (U, \zeta_c, E) be the corresponding vector chart of T(X) (8.1.1) and τ(c′)=(U,ψc,τ(E))\tau(c') = (U, \psi_c, \tau(E)) the corresponding vector chart of F (7.6.2). Put xc=φ(x)x_c = \varphi(x); let ξc\xi_c be the mapping of φ(U)\varphi(U) into E such that ζc(ξ(u))=(u,ξc(φ(u)))\zeta_c(\xi(u)) = (u, \xi_c(\varphi(u))) and fcf_c the mapping of φ(U)\varphi(U) into τ(E)\tau(E) such that ψc(f(u))=(u,fc(φ(u)))\psi_c(f(u)) = (u, f_c(\varphi(u))) for all u∈Uu \in U. Let aca_c be the element (θξc.fc)(xc)(\theta_{\xi_c}.f_c)(x_c) of τ(E)\tau(E) defined in 8.4.2. There exists one and only one element aa of FxF_x such that ψc(a)=(x,ac)\psi_c(a) = (x, a_c) for every chart cc of X at xx. We denote it by (θξ.f)(x)(\theta_{\xi}.f)(x). It depends only on the germs of ξ\xi and ff at xx (and even only on their jet of order 1 (12.1.2)).

The mapping θξ.f:x↦(θξ.f)(x)\theta_{\xi}.f : x \mapsto (\theta_{\xi}.f)(x) is a section of class Cr−1C^{r-1} of F; it depends K-bilinearly on the pair (ξ,f)(\xi, f).

8.4.4. Let us retain the preceding hypotheses and notations. There exists (7.6.4) one and only one morphism of vector bundles τ′\tau' from L(T(X);T(X))\mathscr{L}(T(X); T(X)) into L(F;F)\mathscr{L}(F; F) such that, for every x∈Xx \in X, the restriction of τ′\tau' to the fibre L(T(X);T(X))x=L(Tx(X);Tx(X))\mathscr{L}(T(X); T(X))_x = \mathscr{L}(T_x(X); T_x(X)) is equal to τT(x)′\tau'_{T(x)} (8.4.1). If gg is a function of class CrC^r in XX, with values in KK, we have

θgξ.f=gθξ.f−τ′(dg⊗ξ)(f) \theta_{g\xi}.f = g \theta_\xi.f - \tau'(dg \otimes \xi)(f)
(in this formula, we identify dg⊗ξdg \otimes \xi, which is a section of T′(X)⊗T(X)T'(X) \otimes T(X), with a section of L(T(X);T(X))\mathscr{L}(T(X); T(X)); its image τ′(dg⊗ξ)\tau'(dg \otimes \xi) is a section of L(F;F)\mathscr{L}(F; F) and transforms ff into a section of FF).

8.4.5. Let II be an open set in KK containing 00, UU an open set in XX and φ\varphi a mapping of class CrC^r from I×UI \times U into XX. For (t,x)∈I×U(t, x) \in I \times U, denote by εt,x\varepsilon_{t,x} the vector (1,0)∈K×Tx(X)=T(t,x)(I×U)(1, 0) \in K \times T_x(X) = T_{(t,x)}(I \times U). For t∈It \in I, denote by φt\varphi_t the mapping from UU into XX defined by φt(x)=φ(t,x)\varphi_t(x) = \varphi(t, x) (x∈Ux \in U). We suppose that the following three conditions are satisfied:

a) φ0\varphi_0 is the canonical injection of UU into XX; b) for every t∈Tt \in T, the mapping φt\varphi_t is an isomorphism of CrC^r class manifolds of UU onto an open set of XX; c) the section (t,x)↦T(t,x)(φ)(εt,x)(t, x) \mapsto T_{(t, x)}(\varphi)(\varepsilon_{t, x}) of the vector bundle φ∗T(X)\varphi^*T(X) is of class CrC^r. Moreover, put: d) ξ(x)=T(0,x)(φ)(ε0,x)\xi(x) = T_{(0, x)}(\varphi)(\varepsilon_{0, x}) for every x∈Ux \in U.

The mapping ξ:x↦ξ(x)\xi : x \mapsto \xi(x) is a vector field of class CrC^r on UU. We call it the initial (or starting) vector field of φ\varphi.

Let τ\tau be a vector functor for isomorphisms, of class CrC^r; put F=τ(T(X))F = \tau(T(X)) and let ff be a section of class CrC^r of FF over XX. For x∈Ux \in U and t∈It \in I, put φt∗f(x)=τ(Tx(φt)−1)(f(φt(x)))\varphi_t^*f(x) = \tau(T_x(\varphi_t)^{-1})(f(\varphi_t(x))); this is an element of FxF_x. The mapping t↦φt∗f(x)t \mapsto \varphi_t^*f(x) of II into FxF_x is of class Cr−1C^{r-1} for all x∈Ux \in U and one has

ddt(φt∗f(x))t=0=(θξ.f)(x)pour tout x∈U. \frac{d}{dt} (\varphi_t^*f(x))_{t=0} = (\theta_\xi.f)(x) \quad \text{pour tout } x \in U.

8.4.6. Given a vector field ξ\xi of class CrC^r on XX and a point x0x_0 of XX, there exists an open set II of KK, containing 00, an open set UU of XX containing x0x_0 and a mapping φ:I×U→X\varphi : I \times U \to X of class CrC^r satisfying conditions a),b)a), b) and c) of 8.4.5 and such that the initial field of φ\varphi is the restriction ξ∣U\xi|U of ξ\xi to UU.

8.4.7. Example. — Let FF be a Banach space and let pp be an integer ⩾0\geqslant 0. If VV is a Banach space, put αp(V)=Altp(V;F)\alpha_p(V) = \mathrm{Alt}^p(V; F); if uu is an isomorphism of VV onto a Banach space V′V', denote by αp(u)\alpha_p(u) the isomorphism of αp(V)\alpha_p(V) onto αp(V′)\alpha_p(V') deduced from uu by transport of structure. We thus obtain a vector functor for isomorphisms, denoted by αp\alpha_p (7.8.1 and Errata to No. 7.8). We can apply to it what precedes; we have

αp(T(X))=Altp(T(X);F). \alpha_p(T(X)) = \mathrm{Alt}^p(T(X); F).
The sections of αp(T(X))\alpha_p(T(X)) are the differential forms of degree pp on XX, with values in FF; if ω\omega is such a form and if ξ\xi is a vector field on XX, both of class CrC^r, θξ.ω\theta_\xi.\omega is a differential form of degree pp on XX, with values in FF and of class Cr−1C^{r-1}. We have
θξ.ω=d(i(ξ)ω)+i(ξ)dω \theta_\xi.\omega = d(i(\xi)\omega) + i(\xi)d\omega

and, when r≥2r \geq 2,

θξ⋅dω=d(θξ⋅ω). \theta_\xi \cdot d\omega = d(\theta_\xi \cdot \omega).

When p=0p = 0, the functor αp\alpha_p is the constant vector functor defined by FF; the bundle α0(T(X))\alpha_0(T(X)) is identified with the trivial bundle FXF_X, and the sections of this bundle are identified with the functions on XX with values in FF. If ξ\xi is a vector field of class CrC^r on XX and if f∈Cr(X;F)f \in \mathscr{C}^r(X; F), we have

θξ⋅f=⟨ξ,df⟩=Dξ(f)(8.2.3); \theta_\xi \cdot f = \langle \xi, df \rangle = D_\xi(f) \quad (8.2.3);

it is an element of Cr−1(X;F)\mathscr{C}^{r-1}(X; F).

8.4.8. Let τ\tau and τ1\tau_1 be two vector functors for isomorphisms. A morphism of vector functors h:τ1→τh : \tau_1 \to \tau defines a morphism of vector bundles, also denoted by hh, from τ1(T(X))\tau_1(T(X)) into τ(T(X))\tau(T(X)) (7.6.4), and makes correspond to a section ff of τ1(T(X))\tau_1(T(X)) a section h(f)h(f) of τ(T(X))\tau(T(X)). If ξ\xi is a vector field on XX, and if ff and ξ\xi are of class CrC^r, we have θξ⋅h(f)=h(θξ⋅f)\theta_\xi \cdot h(f) = h(\theta_\xi \cdot f).

More generally, let τ,τ1,…,τd\tau, \tau_1, \ldots, \tau_d be vector functors for isomorphisms and let h:(τ1,…,τd)→τh : (\tau_1, \ldots, \tau_d) \to \tau be a dd-linear morphism (7.6.4). Let fi∈Sτi(T(X))r(X)f_i \in \mathscr{S}_{\tau_i(T(X))}^r(X) (for i=1,…,di = 1, \ldots, d), and let ξ\xi be a vector field of class CrC^r on XX. We have

θξ⋅h(f1,…,fd)=∑1≤i≤dh(f1,…,fi−1,θξ⋅fi,fi+1,…,fd). \theta_\xi \cdot h(f_1, \ldots, f_d) = \sum_{1 \leq i \leq d} h(f_1, \ldots, f_{i-1}, \theta_\xi \cdot f_i, f_{i+1}, \ldots, f_d).

For example, if ff is a section of τ(T(X))\tau(T(X)) and gg a function on XX, with values in KK, both of class CrC^r, we have

θξ⋅(gf)=(θξ⋅g)f+g(θξ⋅f). \theta_\xi \cdot (gf) = (\theta_\xi \cdot g)f + g(\theta_\xi \cdot f).

If ω1\omega_1 and ω2\omega_2 are two differential forms of class CrC^r, with values in Banach spaces F1F_1 and F2F_2 respectively, we have

θξ⋅(ω1∧ω2)=(θξ⋅ω1)∧ω2+ω1∧(θξ⋅ω2), \theta_\xi \cdot (\omega_1 \wedge \omega_2) = (\theta_\xi \cdot \omega_1) \wedge \omega_2 + \omega_1 \wedge (\theta_\xi \cdot \omega_2),

the exterior product being taken with respect to a continuous bilinear mapping of F1×F2F_1 \times F_2 into a Banach space FF.

8.4.9. Let τ\tau be a vector functor for isomorphisms, contravariant (8.2.7), of class CrC^r, φ:X→Y\varphi : X \to Y a morphism of manifolds of class Cr+1C^{r+1}, ξ\xi (resp. η\eta) a vector field of class CrC^r on XX (resp. YY) such that ξ\xi is φ\varphi-related to η\eta (8.2.6). For every section ff of τ(T(Y))\tau(T(Y)), of class CrC^r, we have

φ∗(θη⋅f)=θξ⋅φ∗f. \varphi^*(\theta_\eta \cdot f) = \theta_\xi \cdot \varphi^*f.

8.5. The bracket

Let r∈Nkr \in \mathbf{N}_k and let XX be a manifold of class Cr+1C^{r+1}.

8.5.1. Apply the definitions of No. 8.4 taking for τ\tau the identity functor: τ(V)=V\tau(V) = V for every Banach space VV and τ(u)=u\tau(u) = u for every isomorphism uu of Banach spaces. We then have τ(T(X))=T(X)\tau(T(X)) = T(X). If ξ\xi and η\eta are two vector fields of class CrC^r on XX, we put

(1)

[ξ,η]=θξ⋅η; [\xi, \eta] = \theta_{\xi} \cdot \eta;
this is a vector field of class Cr−1C^{r-1} on XX, called the bracket of ξ\xi and η.8.5.2.Themapping\eta. 8.5.2. The mapping (\xi, \eta) \mapsto [\xi, \eta]isK−bilinearandalternating.If is K-bilinear and alternating. If fand and garefunctionsofclass are functions of class C^ron on X,withvaluesin, with values in K,onehas:(2), one has: (2) [fξ,gη]=fg[ξ,η]+(fDξg)η−(gDηf)ξ. [f\xi, g\eta] = fg[\xi, \eta] + (fD_{\xi}g)\eta - (gD_{\eta}f)\xi. 8.5.3.Let 8.5.3. Let FbeaBanachspace.Onehas(3) be a Banach space. One has (3) D[ξ,η]=Dξ∘Dη−Dη∘Dξ D_{[\xi, \eta]} = D_{\xi} \circ D_{\eta} - D_{\eta} \circ D_{\xi} inthespaceofmappingsfrom in the space of mappings from \mathscr{C}^{r+1}(X; F)into into \mathscr{C}^{r-1}(X; F).If. If r \geqslant 2andif and if \zetaisathirdvectorfieldofclass is a third vector field of class C^ron on X,onehas(4), one has (4) $ [[\xi, \eta], \zeta] = [\xi, [\eta, \zeta]] - [\eta, [\xi, \zeta]] \tag{1} $orequivalently or equivalently [ξ,[η,ζ]]+[η,[ζ,ξ]]+[ζ,[ξ,η]]=0. [\xi, [\eta, \zeta]] + [\eta, [\zeta, \xi]] + [\zeta, [\xi, \eta]] = 0. Moregenerally,if More generally, if r \geqslant 2andif and if \tauisavectorfunctorforisomorphisms,onehas(5) is a vector functor for isomorphisms, one has (5) θ[ξ,η]=θξ∘θη−θη∘θξ \theta_{[\xi, \eta]} = \theta_{\xi} \circ \theta_{\eta} - \theta_{\eta} \circ \theta_{\xi} inthespaceofmappingsfrom in the space of mappings from \mathscr{S}_{F}^{r}(X)into into \mathscr{S}_{F}^{r-2}(X)(with (with F = \tau(T(X))).If). If r \geqslant \infty,thevectorfieldsofclass, the vector fields of class C^ron on XformaK−Liealgebraforthebracket(LIE,I,§1,No.2).8.5.4.Let form a K-Lie algebra for the bracket (LIE, I, § 1, No. 2). 8.5.4. Let EbeaBanachspace, be a Banach space, Uanopensubsetof an open subset of E,, \xiand and \etatwovectorfieldsofclass two vector fields of class C^ron on U,identifiedwithelementsof, identified with elements of \mathscr{C}^r(U; E).Theirbracketisgivenbytheformula:(6). Their bracket is given by the formula: (6) [ξ,η]=Dξη−Dηξ. [\xi, \eta] = D_{\xi}\eta - D_{\eta}\xi. 8.5.5.Let 8.5.5. Let (u^1, \ldots, u^n)beacoordinatesystemof be a coordinate system of Xinanopensubset in an open subset U.Let. Let \xi = \sum a^i \frac{\partial}{\partial u^i}and and \eta = \sum b^i \frac{\partial}{\partial u^i}betwovectorfieldsofclass be two vector fields of class C^ron on U.Put. Put [ξ,η]=∑ci∂∂ui. [\xi, \eta] = \sum c^i \frac{\partial}{\partial u^i}. Onehas(7) One has (7) ci=∑1≤j≤n(aj∂bi∂uj−bj∂ai∂uj). c^i = \sum_{1 \leq j \leq n} \left( a^j \frac{\partial b^i}{\partial u^j} - b^j \frac{\partial a^i}{\partial u^j} \right). 8.5.6.Let 8.5.6. Let \varphi : X \to Ybeamorphismofvarietiesofclass be a morphism of varieties of class C^{r+1},, \xi_1and and \xi_2twovectorfields1Theformula(4)isstillexactifoneassumesonlythatthevectorfields two vector fields 1 The formula (4) is still exact if one assumes only that the vector fields \xi, \eta, \zeta, [\xi, \eta], [\eta, \zeta], [\zeta, \xi]areallofclass are all of class C^1.ofvectorfieldsonX,. of vector fields on X, \eta_1and and \eta_2twovectorfieldsonY,allofclass two vector fields on Y, all of class C^r.If. If \xi_1and and \xi_2are are \varphi−relatedto-related to \eta_1and and \eta_2respectively, respectively, [ \xi_1, \xi_2 ]is is \varphi−relatedto-related to [ \eta_1, \eta_2 ].8.5.7.Let. 8.5.7. Let \omegabeadifferentialformofdegree be a differential form of degree ponX,withvaluesinaBanachspaceFandofclass on X, with values in a Banach space F and of class C^r,andlet, and let \xi_0, \ldots, \xi_pbevectorfieldsofclass be vector fields of class C^ronX.Wehave(8) on X. We have (8) (θξ0⋅ω)(ξ1,…,ξp)=Dξ0ω(ξ1,…,ξp)−∑i=1pω(ξ1,…,[ξ0,ξi],…,ξp) (\theta_{\xi_0} \cdot \omega)(\xi_1, \ldots, \xi_p) = D_{\xi_0} \omega(\xi_1, \ldots, \xi_p) - \sum_{i=1}^p \omega(\xi_1, \ldots, [\xi_0, \xi_i], \ldots, \xi_p) and(9) and (9) dω(ξ0,…,ξp)=∑i=0p(−1)iDξiω(ξ0,…,ξ^i,…,ξp)+∑i<j(−1)i+jω([ξi,ξj],ξ0,…,ξ^i,…,ξ^j,…,ξp). d\omega(\xi_0, \ldots, \xi_p) = \sum_{i=0}^p (-1)^i D_{\xi_i} \omega(\xi_0, \ldots, \hat{\xi}_i, \ldots, \xi_p) + \sum_{i<j} (-1)^{i+j} \omega([\xi_i, \xi_j], \xi_0, \ldots, \hat{\xi}_i, \ldots, \hat{\xi}_j, \ldots, \xi_p). If If \xiand and \etaarevectorfieldsofclass are vector fields of class C^r,wehave(10), we have (10) θξ∘i(η)−i(η)∘θξ=i([ξ,η]) \theta_{\xi} \circ i(\eta) - i(\eta) \circ \theta_{\xi} = i([\xi, \eta]) inthespaceofmappingsfrom in the space of mappings from r\Omega^p(X; F)into into r-1\Omega^{p-1}(X; F).For. For p = 1,formula(9)reads:(11), formula (9) reads: (11) dω(ξ,η)=Dξ⟨η,ω⟩−Dη⟨ξ,ω⟩−⟨[ξ,η],ω⟩. d\omega(\xi, \eta) = D_{\xi} \langle \eta, \omega \rangle - D_{\eta} \langle \xi, \omega \rangle - \langle [\xi, \eta], \omega \rangle. $ ### 8.6. Liftings Let $r \in \mathbf{N}_kandlet and let g : X \to Ybeamorphismofclass be a morphism of class C^{r+1}manifolds.8.6.1.Aliftingof manifolds. 8.6.1. A lifting of ginto into T(Y)isamapping is a mapping \psi : X \to T(Y)suchthatthediagram such that the diagram T(Y)↗ψ↓πX→gY \begin{array}{ccc} & & T(Y) \\ & \nearrow \psi & \downarrow \pi \\ X & \xrightarrow{g} & Y \end{array} iscommutative, is commutative, \pidenotingthecanonicalprojectionof denoting the canonical projection of T(Y)ontoY.Thedataof onto Y. The data of \psiisequivalenttothatofasectionofthevectorbundle is equivalent to that of a section of the vector bundle g^*T(Y)inverseimageby inverse image by gof of T(Y).Thenotionofliftinggeneralizesthatofvectorfield(towhichitreduceswhen. The notion of lifting generalizes that of vector field (to which it reduces when g = \mathrm{Id}_X);animportantpartofthedefinitionsandresultsconcerning); an important part of the definitions and results concerning \theta_{\xi}and and i(\xi)extendstoliftings;weshallrestrictourselvestobrieflyindicatingafewofthem.8.6.2.Let extends to liftings; we shall restrict ourselves to briefly indicating a few of them. 8.6.2. Let \psi : X \to T(Y)bealiftingof be a lifting of g : X \to Y,andlet, and let \omegabeadifferentialformofdegree be a differential form of degree ponY,withvaluesinavectorbundleFwithbaseY.When on Y, with values in a vector bundle F with base Y. When p \geqslant 1,wedenoteby, we denote by i(\psi, \omega)or or i(\psi)\omegaor or i_\psi(\omega)thedifferentialformonX,ofdegree the differential form on X, of degree p - 1,withvaluesin, with values in g^* F,suchthat(1), such that (1) i(ψ,ω)x(v1,…,vp−1)=ωg(x)(ψ(x),Tx(g).v1,…,Tx(g).vp−1) i(\psi, \omega)_x(v_1, \ldots, v_{p-1}) = \omega_{g(x)}(\psi(x), T_x(g).v_1, \ldots, T_x(g).v_{p-1}) forevery for every x \in Xandeveryfamily and every family v_1, \ldots, v_{p-1}ofelementsof of elements of T_x(X).When. When p = 0,weset, we set i(\psi, \omega) = 0.Wesaythat. We say that i(\psi, \omega)istheinteriorproductof is the interior product of \psiand and \omega;if; if \psiand and \omegaareofclass are of class C^r,thesameistrueof, the same is true of i(\psi, \omega).Let. Let F' \times_Y F'' \to FbeapairingofvectorbundlesoverY.For be a pairing of vector bundles over Y. For \omega' \in {}^r\Omega^{p'}(Y; F')and and \omega'' \in {}^r\Omega^{p''}(Y; F''),wehave(2), we have (2) i(ψ)(ω′∧ω′′)=(i(ψ)ω′)∧g∗ω′′+(−1)p′g∗ω′∧i(ψ)ω′′. i(\psi)(\omega' \wedge \omega'') = (i(\psi)\omega') \wedge g^*\omega'' + (-1)^{p'}g^*\omega' \wedge i(\psi)\omega''. 8.6.3.∗Examples∗a)Avectorfield 8.6.3. *Examples* a) A vector field \xionXdefinesalifting on X defines a lifting T(g) \circ \xiof of ginto into T(Y),andwehave:(3), and we have: (3) i(T(g)∘ξ)=i(ξ)∘g∗. i(T(g) \circ \xi) = i(\xi) \circ g^*. b)Avectorfield b) A vector field \etaonYdefinesalifting on Y defines a lifting \eta \circ gof of ginto into T(Y),andwehave:(4), and we have: (4) i(η∘g)=g∗∘i(η). i(\eta \circ g) = g^* \circ i(\eta). c)Moregenerally,let c) More generally, let h : Y \to Zbeamorphismofvarietiesofclass be a morphism of varieties of class C^{r+1}.If. If \psiisaliftingof is a lifting of ginto into T(Y),then, then T(h) \circ \psiisaliftingof is a lifting of h \circ ginto into T(Z)andwehave:(5) and we have: (5) i(T(h)∘ψ)=i(ψ)∘h∗. i(T(h) \circ \psi) = i(\psi) \circ h^*. If If \varphiisaliftingof is a lifting of hinto into T(Z),then, then \varphi \circ gisaliftingof is a lifting of h \circ ginto into T(Z)andwehave:(6) and we have: (6) i(φ∘g)=g∗∘i(φ). i(\varphi \circ g) = g^* \circ i(\varphi). 8.6.4(∗Infinitesimaltransformations∗).Let 8.6.4 (*Infinitesimal transformations*). Let \psibealiftingofclass be a lifting of class C^rof of gandlet and let \omegabeadifferentialformofdegree be a differential form of degree ponY,withvaluesinaBanachspaceF,andofclass on Y, with values in a Banach space F, and of class C^r.ThedifferentialformonX(7). The differential form on X (7) d(i(ψ)ω)+i(ψ)dω d(i(\psi)\omega) + i(\psi)d\omega isofdegree is of degree pandofclass and of class C^{r-1};wedenoteitby; we denote it by \theta_{\psi}.\omega.If. If fisafunctionofclass is a function of class C^ronX,wehave(8) on X, we have (8) θfψ.ω=df∧i(ψ)ω+fθψ.ω. \theta_{f\psi}.\omega = df \wedge i(\psi)\omega + f\theta_{\psi}.\omega. 8.6.5(∗Characterizationof 8.6.5 (*Characterization of \theta_{\psi}.\omegaasaderivative∗).Retainthehypothesesof8.6.4.Let as a derivative*). Retain the hypotheses of 8.6.4. Let x \in X.TherethenexistsanopenneighbourhoodUof. There then exists an open neighbourhood U of x,anopenneighbourhoodIof0inK,andamorphism, an open neighbourhood I of 0 in K, and a morphism G : I \times U \to Y,ofclass, of class C^r,havingthefollowingtwoproperties:a)Forevery, having the following two properties: a) For every x \in U,wehave, we have G(0, x) = g(x).b)Forevery. b) For every x \in U,theimageby, the image by T_{(0, x)}(G)ofthetangentvector of the tangent vector (1, 0)isequalto is equal to \psi(x).Supposethat(U,I,G)satisfiestheseconditions;forevery. Suppose that (U, I, G) satisfies these conditions; for every t \in I,denoteby, denote by G_tthemapping the mapping x \mapsto G(t, x)fromXintoY;put from X into Y; put \omega_t = G_t^*(\omega).Forevery. For every x \in X,themapping, the mapping t \mapsto \omega_t(x)fromIinto from I into \mathrm{Alt}^p(T_x(X), F)isofclass is of class C^r,anditsderivativeattheoriginisgivenbytheformula, and its derivative at the origin is given by the formula ddt(ωt(x))t=0=(θψ⋅ω)(x). \frac{d}{dt} (\omega_t(x))_{t=0} = (\theta_\psi \cdot \omega)(x). $ ### 8.7. Weakening of structure In this no., we suppose $K = \mathbf{R}.8.7.1.LetXbeamanifoldofclass. 8.7.1. Let X be a manifold of class C^s,andletFbeavectorbundleoverX,ofclass, and let F be a vector bundle over X, of class C^k,with, with 0 \leq k \leq s.If. If 0 \leq k' \leq k,thereexistsonFoneandonlyonestructure, there exists on F one and only one structure F_{k'}ofvectorbundlewithbaseXandofclass of vector bundle with base X and of class C^{k'}suchthateveryvectorbundlechartofFisavectorbundlechartof such that every vector bundle chart of F is a vector bundle chart of F_{k'}.Wesaythat. We say that F_{k'}isobtainedfromFbyweakeningthebundlestructureofF.8.7.2.Let is obtained from F by weakening the bundle structure of F. 8.7.2. Let r \in \mathbf{N}_\mathbf{R}with with r \leq s,andlet, and let X_rbethemanifoldofclass be the manifold of class C^runderlyingX(5.13.1).Thetangentbundle underlying X (5.13.1). The tangent bundle T(X_r)isofclass is of class C^{r-1};itisthebundleobtainedbyweakeningthestructurefromthetangentbundle; it is the bundle obtained by weakening the structure from the tangent bundle T(X),whichisofclass, which is of class C^{s-1}.LetFbeavectorbundleoverX,ofclass. Let F be a vector bundle over X, of class C^k,for, for 0 \leq k \leq r - 1.Thedifferentialformsofclass. The differential forms of class C^konXwithvaluesinFarecanonicallyidentifiedwiththecorrespondingdifferentialformson on X with values in F are canonically identified with the corresponding differential forms on X_r$. The various operations on these forms described in the remainder of this paragraph are compatible with this identification. In what follows in this fascicle, we shall often leave it to the reader to make explicit the other results of this kind. ### 8.8. Almost complex manifolds and complex manifolds In this no., we suppose $K = \mathbf{R}anddenotebyXa(real)manifoldofclass and denote by X a (real) manifold of class C^r,with, with r \in \mathbf{N}_\mathbf{R}.8.8.1(«Complexvectorbundles»).AvectorbundleoverCwithbaseX(7.3.4)isalsocalledacomplexvectorbundlewithbaseX.IfMissuchavectorbundle,wecallacomplexvectorbundlechartofMatriple. 8.8.1 (« Complex vector bundles »). A vector bundle over C with base X (7.3.4) is also called a complex vector bundle with base X. If M is such a vector bundle, we call a complex vector bundle chart of M a triple (U, \varphi, E),whereUisanopensetinX,EacomplexBanachspaceand, where U is an open set in X, E a complex Banach space and \varphianisomorphismofcomplexvectorbundlesof an isomorphism of complex vector bundles of M|Uontothetrivialbundle onto the trivial bundle E_U = U \times E.Afamily. A family (U_i, \varphi_i, E_i)ofcomplexvectorbundlechartsofMwhosedomainsofdefinition of complex vector bundle charts of M whose domains of definition U_icoverXiscalledacomplexvectorbundleatlasofM;everycomplexvectorbundlepossessesacomplexvectorbundleatlas(7.3.3).WesometimessayC−vectorialinsteadofcomplexvectorial.Analogously,wesometimessay,whenwewishtospeakofavectorbundleover cover X is called a complex vector bundle atlas of M; every complex vector bundle possesses a complex vector bundle atlas (7.3.3). We sometimes say C-vectorial instead of complex vectorial. Analogously, we sometimes say, when we wish to speak of a vector bundle over \mathbf{R},ofanordinaryvectorbundlechartofthisbundle,etc.,«realvectorial»or«R−vectorial»insteadof«vectorial».LetMbeacomplexvectorbundlewithbaseX.Thereexistsoneandonlyoneautomorphism, of an ordinary vector bundle chart of this bundle, etc., « real vectorial » or « R-vectorial » instead of « vectorial ». Let M be a complex vector bundle with base X. There exists one and only one automorphism joftheunderlying(real)vectorbundleofM(7.3.3)whoserestrictiontoeachfibreismultiplicationbytheelementiofC;thesquareofjisequalto−1.Conversely,ifMisa(real)vectorbundlewithbaseXandjanautomorphismofMsuchthat of the underlying (real) vector bundle of M (7.3.3) whose restriction to each fibre is multiplication by the element i of C; the square of j is equal to −1. Conversely, if M is a (real) vector bundle with base X and j an automorphism of M such that j^2 = -1,thereexistsonMauniquestructureofcomplexvectorbundleadmittingMasitsunderlying(real)vectorbundleandforwhichjismultiplicationbyi.8.8.2(«Complexificationofavectorbundle»).Wedefineavectorialfunctorτbysetting, there exists on M a unique structure of complex vector bundle admitting M as its underlying (real) vector bundle and for which j is multiplication by i. 8.8.2 (« Complexification of a vector bundle »). We define a vectorial functor τ by setting \tau(E) = E \otimes \mathbf{C}forevery(real)BanachspaceE,and for every (real) Banach space E, and \tau(u) = u \otimes \mathrm{Id}_\mathbf{C}foreverymorphism for every morphism u : E \to E'of(real)Banachspaces.If of (real) Banach spaces. If Fisavectorbundlewithbase is a vector bundle with base Xandofclass and of class C^k( (0 \leq k \leq r),itstransformbythevectorbundlefunctor), its transform by the vector bundle functor \tauisdenoted is denoted F \otimes \mathbf{C}.Thereexistson. There exists on F \otimes \mathbf{C}auniquestructureofcomplexvectorbundlewithbase a unique structure of complex vector bundle with base Xandofclass and of class C^k,compatiblewithitsstructureasa(real)vectorbundleandinducingoneachfibre, compatible with its structure as a (real) vector bundle and inducing on each fibre (F \otimes \mathbf{C})_x = F_x \otimes \mathbf{C}itscanonicalstructureasacomplexBanachspace(EVT,II,§8,No.1,Example).Endowedwiththisstructure, its canonical structure as a complex Banach space (EVT, II, § 8, No. 1, Example). Endowed with this structure, F \otimes \mathbf{C}iscalledthecomplexificationof is called the complexification of F.Let. Let Ubeanopensubsetof be an open subset of X;thecanonicalmapping; the canonical mapping SFk(U)⊗C→SF⊗Ck(U) \mathscr{S}_F^k(U) \otimes \mathbf{C} \to \mathscr{S}_{F \otimes \mathbf{C}}^k(U) isanisomorphism,bywhichthesetwospacesareidentified.If is an isomorphism, by which these two spaces are identified. If s \in \mathscr{S}_{F \otimes \mathbf{C}}^k(U),theelements, the elements \sigma, \tauof of \mathscr{S}_F^k(U)suchthat such that s = \sigma + i \tauarecalledtherealpartandtheimaginarypartof are called the real part and the imaginary part of s;thesection; the section \bar{s} = \sigma - i \tauiscalledtheconjugateof is called the conjugate of s.

In particular, a section of the bundle T(X)⊗CT(X) \otimes \mathbf{C} is called a complex vector field on XX.

Let HH be a complex vector bundle with base XX. The canonical isomorphisms AltRp(Tx(X);H)→AltCp(Tx(X)⊗C;H)\mathrm{Alt}_\mathbf{R}^p(T_x(X); H) \to \mathrm{Alt}_\mathbf{C}^p(T_x(X) \otimes \mathbf{C}; H) define an isomorphism of complex vector bundles, called canonical, of AltRp(T(X);H)\mathrm{Alt}_\mathbf{R}^p(T(X); H) onto AltCp(T(X)⊗C;H)\mathrm{Alt}_\mathbf{C}^p(T(X) \otimes \mathbf{C}; H) (7.8.5), by means of which we shall identify these two bundles. Let ω\omega be a section of this bundle, in other words a differential form of degree p on XX, with values in HH, and let ζ\zeta be a complex vector field, with real part ξ\xi and imaginary part η\eta. We then put:

i(ζ,ω)=i(ξ,ω)+i.i(η,ω). i(\zeta, \omega) = i(\xi, \omega) + i.i(\eta, \omega).

If HH is a trivial bundle, we put

θζ.ω=θξ.ω+iθη.ω. \theta_\zeta.\omega = \theta_\xi.\omega + i \theta_\eta.\omega.

Analogously, we extend the bracket by linearity to complex vector fields. The formulas of the preceding Nos. remain valid.

8.8.3. A structure of class CkC^k (k≤r−1k \leq r - 1) on XX is called an almost complex structure if it is the datum of a complex vector bundle structure on T(X)T(X), of class CkC^k, whose underlying real structure is the natural structure of T(X)T(X). Such a structure is equivalent to the datum of an automorphism j of class CkC^k of T(X)T(X) such that j2=−1j^2 = -1.

Let us give ourselves such a structure. Extend j to a C\mathbf{C}-automorphism of T(X)⊗CT(X) \otimes \mathbf{C}. There exists one and only one decomposition of T(X)⊗CT(X) \otimes \mathbf{C} into a direct sum of two complex subbundles:

(1)

T(X)⊗C=T′(X)⊕T′′(X) T(X) \otimes \mathbf{C} = T'(X) \oplus T''(X)

such that jj coincides with multiplication by ii on T′(X)T'(X) and by −i-i on T′′(X)T''(X). The projector p′p' of T(X)⊗CT(X) \otimes \mathbf{C} onto T′(X)T'(X) is equal to 12(1−ij)\frac{1}{2}(1 - ij); the projector p′′=1−p′p'' = 1 - p' of T(X)⊗CT(X) \otimes \mathbf{C} onto T′′(X)T''(X) is equal to 12(1+ij)\frac{1}{2}(1 + ij). The composites

π′:T(X)→T(X)⊗C→p′T′(X) \pi': \quad T(X) \to T(X) \otimes \mathbf{C} \xrightarrow{p'} T'(X)
π′′:T(X)→T(X)⊗C→p′′T′′(X) \pi'': \quad T(X) \to T(X) \otimes \mathbf{C} \xrightarrow{p''} T''(X)
are R\mathbf{R}-isomorphisms; the first transforms jj into multiplication by ii, the second into multiplication by −i-i.

8.8.4 (“Forms of type (p,q)(p, q)”). Retain the hypotheses and notations of the preceding no. Let FF be a complex vector bundle with base XX, let pp and qq be two integers ⩾0\geqslant 0, and let n=p+qn = p + q. Let ω\omega be a differential form of degree nn on an open set UU of XX, with values in FF; identify (8.8.2) ω\omega with a section of Altcn(T(X)⊗C;F)\mathrm{Alt}_c^n(T(X) \otimes \mathbf{C}; F). We say that ω\omega is of type (p,q)(p, q) if, for every x∈Ux \in U, one has

ωx(v1,…,vn)=0 \omega_x(v_1, \ldots, v_n) = 0
as soon as p+1p + 1 of the vectors viv_i belong to Tx′(X)T'_x(X) or q+1q + 1 of the vectors viv_i belong to Tx′′(X)T''_x(X). If one identifies ⋀nTx(X)⊗C\bigwedge^n T_x(X) \otimes \mathbf{C} with the direct sum of the spaces ⋀m′Tx′(X)⊗⋀m′′Tx′′(X)\bigwedge^{m'} T'_x(X) \otimes \bigwedge^{m''} T''_x(X) for m′+m′′=nm' + m'' = n (A, III, p. 85) and ωx\omega_x with a C\mathbf{C}-linear form on ⋀nTx(X)\bigwedge^n T_x(X), it amounts to saying that ωx\omega_x is zero on ⋀m′Tx′(X)⊗⋀m′′Tx′′(X)\bigwedge^{m'} T'_x(X) \otimes \bigwedge^{m''} T''_x(X) for (m′,m′′)≠(p,q)(m', m'') \neq (p, q).

For every pair (p,q)(p, q) of integers ⩾0\geqslant 0 with p+q=np + q = n, there exists one and only one complex vector subbundle Altp,q(T(X);F)\mathrm{Alt}^{p,q}(T(X); F) of Altn(T(X);F)\mathrm{Alt}^n(T(X); F) such that its sections on an open set UU of XX are the differential forms of type (p,q)(p, q) on XX, with values in FF. The vector bundle Altn(T(X);F)\mathrm{Alt}^n(T(X); F) is the direct sum of the vector bundles Altp,q(T(X);F)\mathrm{Alt}^{p,q}(T(X); F) for p⩾0, q⩾0p \geqslant 0,\ q \geqslant 0 and p+q=np + q = n. Every differential form ω\omega of degree nn with values in FF decomposes uniquely into

ω=∑p+q=nωp,q \omega = \sum_{p+q=n} \omega_{p,q}
where ωp,q\omega_{p,q} is a form of type (p,q)(p, q), called the component of type (p,q)(p, q) of ω\omega. If ω\omega is of class Ch\mathbf{C}^h, with 0≤h≤k0 \leq h \leq k, the same is true of its components.

Examples

(a) A differential form of degree nn is of type (n,0)(n, 0) if and only if it is C\mathbf{C}-multilinear.

(b) Let F′,F′′F', F'' and FF be three complex vector bundles and let F′×XF′′→FF' \times_X F'' \to F be a C\mathbf{C}-bilinear pairing. If ω′\omega' (resp. ω′′\omega'') is a differential form of type (p′,q′)(p', q') (resp. (p′′,q′′)(p'', q'')) with values in F′F' (resp. F′′F''), the differential form ω′∧ω′′\omega' \wedge \omega'' is of type (p′+p′′,q′+q′′)(p' + p'', q' + q'').

(c) Suppose that FF is the complexification of a (real) vector bundle (8.8.2). If ω\omega is a differential form of type (p,q)(p, q) with values in FF, its conjugate ω‾\overline{\omega} (8.8.2) is of type (q,p)(q, p).

8.8.5. In addition to the preceding hypotheses, suppose that k⩾1k \geqslant 1. The following three conditions are then equivalent:

(i) For every open set U of X and for every pair (ξ,η)(\xi, \eta) of complex vector fields on U, of class CkC^k, such that ξ(x)\xi(x) and η(x)\eta(x) belong to Tx′(X)T'_x(X) for every x∈Ux \in U, one has [ξ,η](x)∈Tx′(X)[\xi, \eta](x) \in T'_x(X) for every x∈Ux \in U.

(ii) For every open set U of X and every pair (ξ,η)(\xi, \eta) of (real) vector fields on U, of class CkC^k, one has

[ξ,η]+j[jξ,η]+j[ξ,jη]−[jξ,jη]=0. [\xi, \eta] + j[j\xi, \eta] + j[\xi, j\eta] - [j\xi, j\eta] = 0.

(iii) For every open set U of X and for every complex differential form ω\omega of type (1,0)(1, 0) on U, of class CkC^k, the component of type (0,2)(0, 2) of dωd\omega is zero.

Suppose that these conditions are satisfied. Let ω\omega be a differential form of type (p,q)(p, q) on an open set U of X, of class ChC^h with 1≤h≤k1 \leq h \leq k, with values in a complex Banach space F. We denote by d′ωd'\omega (resp. d′′ωd''\omega) the component of type (p+1,q)(p+1, q) (resp. (p,q+1)(p, q+1)) of dωd\omega; the other components of dωd\omega are then zero and we have

dω=d′ω+d′′ω. d\omega = d'\omega + d''\omega.
If k≥2k \geq 2, we have
d′(d′ω)=0,d′′(d′′ω)=0,d′(d′′ω)+d′′(d′ω)=0. d'(d'\omega) = 0 \quad , \quad d''(d''\omega) = 0 \quad , \quad d'(d''\omega) + d''(d'\omega) = 0.
With the notation of 8.8.4, example b), we have
d′(ω′∧ω′′)=d′(ω′)∧ω′′+(−1)p′+q′ω′∧d′(ω′′) d'(\omega' \wedge \omega'') = d'(\omega') \wedge \omega'' + (-1)^{p'+q'} \omega' \wedge d'(\omega'')
d′′(ω′∧ω′′)=d′′(ω′)∧ω′′+(−1)p′+q′ω′∧d′′(ω′′). d''(\omega' \wedge \omega'') = d''(\omega') \wedge \omega'' + (-1)^{p'+q'} \omega' \wedge d''(\omega'').
With that of 8.8.4, example c), we have
d′(ω‾)=d′′(ω)‾. d'(\overline{\omega}) = \overline{d''(\omega)}.
In formulas (4) and (5) (resp. (6)), the differential forms ω′\omega' and ω′′\omega'' (resp. ω\omega) are assumed to be of class C1C^1.

8.8.6 (« Almost complex structure of a complex manifold »). Let XcX^c be a complex analytic manifold, having X as underlying real analytic manifold (5.14.2.a)). The bundle T(X)T(X) is identified with the underlying (real) vector bundle of the complex vector bundle T(Xc)T(X^c), which endows X with an almost complex structure of class CωC^\omega, said to be defined by the complex analytic manifold structure given on X. This almost complex structure satisfies conditions (i) to (iii) of 8.8.5; in particular, the operators d′d' and d′′d'' of 8.8.5 are defined. If f:Xc→Ycf : X^c \to Y^c is a morphism of complex analytic manifolds, f∗f^* commutes with the operators d′d' and d′′d''.

8.8.7. Retain the hypotheses and notations of 8.8.6. Let X‾c\overline{X}^c be the conjugate of XcX^c (5.14.2.b)). Embed X by the diagonal mapping x↦(x,x)x \mapsto (x, x) in the complex manifold Xc×X‾cX^c \times \overline{X}^c, and let g be the anti-automorphism (x,y)↦(y,x)(x, y) \mapsto (y, x) of Xc×X‾cX^c \times \overline{X}^c. The pair (Xc×X‾c,g)(X^c \times \overline{X}^c, g) is a complexification of X (5.14.8). In particular, for every x∈Xx \in X, the tangent space Tx(Xc×X‾c)T_x(X^c \times \overline{X}^c) is identified with Tx(X)⊗CT_x(X) \otimes \mathbf{C}; under this identification, Tx(Xc×{x})T_x(X^c \times \{x\}) corresponds to Tx′(X)T'_x(X) and Tx({x}×X‾c)T_x(\{x\} \times \overline{X}^c) corresponds to Tx′′(X)T''_x(X).

8.8.8. Suppose r=ωr = \omega; every almost complex structure of class CωC^\omega on XX satisfying the equivalent conditions (i) to (iii) of 8.8.5 is the almost complex structure defined by one and only one complex analytic manifold structure on XX.¹

8.8.9 (« Holomorphic forms »). Let us take up the hypotheses and notations of 8.8.6, and let FF be a complex Banach space. Morphic (in other words complex analytic) differential forms on XcX^c, with values in FF, are also called holomorphic differential forms; the identification of T(Xc)T(X^c) with T(X)T(X) identifies them with (real analytic) differential forms on XX. For a differential form ω\omega of degree pp on XX, with values in FF and of class CkC^k with k⩾1k \geqslant 1, to be holomorphic, it is necessary and sufficient that it be of type (p,0)(p, 0) and that d′′ω=0d''\omega = 0.

Let ξ\xi be a vector field on XX. We say that ξ\xi is holomorphic if it is a complex analytic mapping of XcX^c into T(Xc)=T(X)T(X^c) = T(X), in other words a complex analytic vector field on XcX^c. If this is the case, and if ω\omega is a holomorphic differential form on XX with values in FF, the form θξ.ω\theta_\xi.\omega (resp. i(ξ)ωi(\xi)\omega) is the same, whether we consider ξ\xi as a complex analytic vector field on XcX^c and ω\omega as an element of Ωp(Xc;F)\Omega^p(X^c; F), or ξ\xi as a vector field on XX and ω\omega as an element of Ωp(X;F)\Omega^p(X; F). Moreover, let ξ′=π′(ξ)\xi' = \pi'(\xi) and ξ′′=π′′(ξ)\xi'' = \pi''(\xi) be the components of ξ\xi in T′(X)T'(X) and T′′(X)T''(X) respectively (8.8.3); we have

θξ.ω=θξ′.ω,θξ′′.ω=0(7) \theta_\xi.\omega = \theta_{\xi'}.\omega \quad , \quad \theta_{\xi''}.\omega = 0 \tag{7}
i(ξ)ω=i(ξ′)ω,i(ξ′′)ω=0.(8) i(\xi)\omega = i(\xi')\omega \quad , \quad i(\xi'')\omega = 0. \tag{8}

8.8.10. Example. — Suppose that XcX^c is an open set in Cn\mathbf{C}^n and denote by z1,…,znz^1, \ldots, z^n the coordinate functions on XcX^c. For 1⩽k⩽n1 \leqslant k \leqslant n, put zk=xk+iykz^k = x^k + iy^k, where xkx^k and yky^k are real-valued. Consider the tangent frame (∂/∂zk)(\partial/\partial z^k) of T(Xc)T(X^c) defined by the coordinate system (zk)(z^k) and the tangent frame (∂/∂xk,∂/∂yk)(\partial/\partial x^k, \partial/\partial y^k) of T(X)T(X) defined by the coordinate system (xk,yk)(x^k, y^k) (8.1.5). We have j(∂/∂xk)=∂/∂ykj(\partial/\partial x^k) = \partial/\partial y^k and the image of ∂/∂zk\partial/\partial z^k by the mapping π′:T(X)=T(Xc)→T′(X)\pi': T(X) = T(X^c) \to T'(X) (8.8.3) is equal to

12(∂/∂xk−i∂/∂yk); \frac{1}{2}(\partial/\partial x^k - i \partial/\partial y^k);
we shall still denote it in general by ∂/∂zk\partial/\partial z^k.² The complex conjugate vector field of this field ∂/∂zk\partial/\partial z^k is denoted by ∂/∂zˉk\partial/\partial \bar{z}^k; we have
∂/∂zˉk=12(∂/∂xk+i∂/∂yk).(9) \partial/\partial \bar{z}^k = \frac{1}{2}(\partial/\partial x^k + i \partial/\partial y^k). \tag{9}

If ff is a function of class C1C^1 on XX, with values in a complex Banach space FF, the differential forms d′fd'f and d′′fd''f (8.8.5) are given by

d′f=∑1⩽k⩽n∂f∂zk dzk,d′′f=∑1⩽k⩽n∂f∂zˉk dzˉk.(10) d'f = \sum_{1 \leqslant k \leqslant n} \frac{\partial f}{\partial z^k} \, dz^k \quad , \quad d''f = \sum_{1 \leqslant k \leqslant n} \frac{\partial f}{\partial \bar{z}^k} \, d\bar{z}^k. \tag{10}

¹ If XX is finite-dimensional, this remains true for an almost complex structure of class CkC^k with k⩾dim⁡Xk \geqslant \dim X (cf. A. NEWLANDER and L. NIRENBERG, Complex analytic coordinates in almost complex manifolds, Ann. of Math. LXV (1957), p. 391–404). ² Care must be taken that the canonical identification of T(Xc)T(X^c) with T(X)T(X) does not transform the vector field ∂/∂zk\partial/\partial z^k on XcX^c into the vector field ∂/∂zk\partial/\partial z^k on XX, but into the vector field ∂/∂zk+∂/∂zˉk\partial/\partial z^k + \partial/\partial \bar{z}^k. However, the two vector fields denoted by ∂/∂zk\partial/\partial z^k take the same value on holomorphic differential forms (8.8.9), which are moreover the only forms to which a vector field of XcX^c can be applied.

Let us recall that we have

df=d′f+d′′f df = d'f + d''f
dzk=dxk+i dykdzˉk=dxk−i dyk. dz^k = dx^k + i\ dy^k \qquad d\bar{z}^k = dx^k - i\ dy^k.

If A=(i1,…,ip)A = (i_1, \ldots, i_p) is a strictly increasing sequence of integers belonging to the interval [1,n][1, n], put

dzA=dzi1∧⋯∧dzip dz^A = dz^{i_1} \wedge \cdots \wedge dz^{i_p}

and denote by dzˉAd\bar{z}^A the conjugate of dzAdz^A. Every differential form ω\omega of type (p,q)(p, q) with values in FF can be written uniquely

(11)

ω=∑A,BfA,B dzA∧dzˉB \omega = \sum_{A, B} f_{A, B}\ dz^A \wedge d\bar{z}^B

where AA (resp. BB) runs through the set of strictly increasing sequences of pp (resp. qq) elements of [1,n][1, n], the fA,Bf_{A, B} being functions with values in FF. If ω\omega is of class CkC^k, with k⩾1k \geqslant 1, the same is true of the functions fA,Bf_{A, B} and we have

(12)

d′ω=∑A,Bd′fA,B∧dzA∧dzˉB d'\omega = \sum_{A, B} d'f_{A, B} \wedge dz^A \wedge d\bar{z}^B

(13)

d′′ω=∑A,Bd′′fA,B∧dzA∧dzˉB. d''\omega = \sum_{A, B} d''f_{A, B} \wedge dz^A \wedge d\bar{z}^B.

[^1]: When K=RK=\mathbf{R} and r=1r=1, T(X)T(X) is a topological vector bundle (cf. Notations and conventions).

Machine translation of the English, by gpt-5-6, gpt-5-6-mini, against glossary version 34. Not checked by a person. That model is a cut down version of the one the rest of this language was written by.