Bourbaki

§ 10. Measures defined by differential forms

In this paragraph, it is assumed that KK is locally compact. Starting with No. 10.2, it is assumed that K=RK=\mathbf{R}. In Nos. 10.1 and 10.4, all the varieties considered are assumed to be locally finite-dimensional; when they are separated, they are locally compact.

10.1. Module measure of a differential form

Notations. — We denote by μ\mu a Haar measure (INT, VII, § 1, No. 2) on the additive group of KK. We denote by μ⊗n\mu^{\otimes n} the measure μ⊗⋯⊗μ\mu\otimes\cdots\otimes\mu on KnK^n and by μU⊗n\mu^{\otimes n}_U its restriction to an open subset UU of KnK^n. For a∈Ka\in K, we denote by mod⁡(a)\operatorname{mod}(a) the module of aa (INT, VII, § 1, No. 10 and AC, VI, § 9, No. 1). If K=RK=\mathbf{R}, we have mod⁡(a)=∣a∣\operatorname{mod}(a)=|a|; if K=CK=\mathbf{C}, we have mod⁡(a)=∣a∣2\operatorname{mod}(a)=|a|^2; if KK is ultrametric, we have mod⁡(a)=q−ν(a)\operatorname{mod}(a)=q^{-\nu(a)}, where qq denotes the number of elements of the residue field of KK and ν\nu the named valuation of KK (AC, VI, § 9, No. 1, prop. 1).

10.1.1. Let UU and VV be open subsets of KnK^n, and let f:U→Vf:U\to V be a mapping of class CrC^r, with r∈Nr\in\mathbf{N}. Let x∈Ux\in U; the Jacobian of ff at xx, denoted by Jac⁡x(f)\operatorname{Jac}_x(f), is called the determinant of the linear mapping Df(x)Df(x) derived from ff at xx. We denote by Jac⁡(f)\operatorname{Jac}(f) the function x↦Jac⁡x(f)x\mapsto\operatorname{Jac}_x(f); the function mod⁡(Jac⁡(f))\operatorname{mod}(\operatorname{Jac}(f)) is a continuous function in UU with positive real values.

10.1.2 (« Change of variable in integrals »). Under the hypotheses of 10.1.1, suppose that ff is an isomorphism of class CrC^r of the variety UU onto the variety VV. Then the image by ff of the measure mod⁡(Jac⁡(f))μU⊗n\operatorname{mod}(\operatorname{Jac}(f))\mu^{\otimes n}_U is μV⊗n\mu^{\otimes n}_V; for every continuous function with compact support φ:V→C\varphi:V\to\mathbf{C}, we have

∫Vφ(y)μ⊗n(y)=∫Uφ(f(x)).mod⁡(Jac⁡x(f))μ⊗n(x). \int_V \varphi(y)\mu^{\otimes n}(y)=\int_U \varphi(f(x)).\operatorname{mod}(\operatorname{Jac}_x(f))\mu^{\otimes n}(x).

10.1.3. Let XX be a variety of class CrC^r, and let AA be a subset of XX. We say that AA is locally negligible if, for every chart (U,φ,Kn)(U,\varphi,K^n) of the variety XX, the set φ(A∩U)\varphi(A\cap U) is μ⊗n\mu^{\otimes n}-negligible (INT, IV, § 2, No. 2); this condition does not depend on the choice of μ\mu, and it is sufficient to verify it for a family of charts whose domains cover AA. Every set contained in the union of a countable family of locally negligible sets is locally negligible.

Examples

a) Any subvariety of X which is of codimension ≥1\geq 1 at every point (i.e. of empty interior) is locally negligible.

b) Let g be a function of class CrC^r on X, and let AgA_g be the set of points x∈Xx \in X such that g(x)=0g(x) = 0; suppose that the interior of AgA_g is empty, and that r=ωr = \omega; then AgA_g is locally negligible.

c) Let f:Y→Xf : Y \to X be a morphism of varieties of class CrC^r, the variety Y being a countable union of compact subsets. Suppose that one has dim⁡yY≤dim⁡f(y)X\dim_y Y \leq \dim_{f(y)} X for every y∈Yy \in Y. The image by ff of every locally negligible subset of Y is a locally negligible subset of X. The same is true of the image by ff of the set of points where ff is not étale ("first theorem of Sard"); in particular, if dim⁡yY<dim⁡f(y)X\dim_y Y < \dim_{f(y)} X for every y∈Y,f(Y)y \in Y, f(Y) is a locally negligible subset of X.

d) Suppose that K is of characteristic zero. Let f:Y→Xf : Y \to X be a morphism of varieties of class CrC^r (r∈NK,r≥∞r \in \mathbf{N}_K, r \geq \infty), Y being a countable union of compact subsets. Let C be the set of points of Y where ff is not a submersion ("critical points"). Then f(C)f(C) is a locally negligible subset of X ("second theorem of Sard").[^1]

10.1.4. Let X be a paracompact variety of class CrC^r. There exists on X a class M of equivalent measures (INT, V, § 5, No. 6) and only one such that, for every ν∈M\nu \in M and every chart c=(U,φ,Kn)c = (U, \varphi, K^n) of X, the image by φ\varphi of the restriction of ν\nu to U is equivalent to μφ(U)⊗n\mu_{\varphi(U)}^{\otimes n}. The class M is called the canonical class of measures on X. For a subset A of X to be locally negligible (10.1.3), it is necessary and sufficient that it be locally negligible (INT, IV, § 2, No. 2) for one (resp. every) measure ν∈M\nu \in M.

If K=RK = \mathbf{R} and r≠ωr \neq \omega (resp. K=RK = \mathbf{R} or CC and r=ωr = \omega, resp. K is ultrametric), there exists ν∈M\nu \in M such that, for every chart c=(U,φ,Kn)c = (U, \varphi, K^n) of X, the density of φ(νU)\varphi(\nu_U) with respect to μφ(U)⊗n\mu_{\varphi(U)}^{\otimes n} is everywhere >0> 0 and of class Cr−1C^{r-1} (resp. of class C∞C^\infty, resp. locally constant). If ν\nu and ν′\nu' are two such measures, the density of ν′\nu' with respect to ν\nu is everywhere >0> 0 and of class Cr−1C^{r-1} (resp. of class C∞C^\infty, resp. locally constant).

10.1.5. Let XX be a variety of class CrC^r; let T′(X)T'(X) be the cotangent bundle of X (8.2.2) and put Ω=det⁡(T′(X))\Omega = \det(T'(X)) (7.9.9). The vector bundle Ω\Omega is of rank 1 at each point; when X is pure of dimension nn, it is identified with the vector bundle Altn(T(X);KX)\mathrm{Alt}^n(T(X); K_X). Let ω\omega be a section of Ω\Omega on X; one says, by abuse of language, that ω\omega is a differential form of maximum degree on X. Let c=(U,φ,Kn)c = (U, \varphi, K^n) be a chart of X; denote by u1,…,unu^1, \ldots, u^n the coordinate functions on KnK^n. There exists one and only one function fcf_c on φ(U)\varphi(U) such that ω∣U=φ∗(fcdu1∧⋯∧dun)\omega|U = \varphi^*(f_c du^1 \wedge \cdots \wedge du^n). One says that ω\omega is locally of integrable modulus if, for every chart c=(U,φ,Kn)c = (U, \varphi, K^n) of X, the real function mod(fc):φ(U)→R\mathrm{mod}(f_c) : \varphi(U) \to \mathbf{R} is locally integrable for μφ(U)⊗n\mu_{\varphi(U)}^{\otimes n} (INT, IV, § 4, No. 1); it suffices to verify this property for the charts of an atlas of X. If ω\omega is continuous, and in particular if ω\omega is of class CsC^s, with s∈NK,s≤r−1s \in \mathbf{N}_K, s \leq r - 1, then ω\omega is locally of integrable modulus.

10.1.6 (“Positive measure defined by a differential form of maximum degree”). Retain the notation of 10.1.5 and suppose in addition that X is separated and that ω\omega is locally of integrable modulus. If c=(U,φ,Kn)c = (U, \varphi, K^n) is a chart of X, denote by νc\nu_c the measure on φ(U)\varphi(U) product of the measure μφ(U)⊗n\mu_{\varphi(U)}^{\otimes n} by the function mod(fc)(f_c) (INT, V, § 5, No. 2, def. 2) and let αc\alpha_c be the image of νc\nu_c by φ−1\varphi^{-1}. There exists on X one and only one measure α\alpha such that, for every chart c=(U,φ,Kn)c = (U, \varphi, K^n) of X, the restriction of α\alpha to U is equal to αc\alpha_c. One says that the measure α\alpha is the modulus of ω\omega and denotes it by mod(ω)μ(\omega)_\mu. It is a positive measure. When K=RK = \mathbf{R} and μ\mu is Lebesgue measure, one writes ∣ω∣|\omega| instead of mod(ω)μ(\omega)_\mu.

If X is pure of dimension nn, and if aa is a real number >0> 0, one has mod(ω)aμ=anmod(ω)μ\mathrm{mod}(\omega)_{a\mu} = a^n \mathrm{mod}(\omega)_\mu.

Let A be a subset of X. In order that A be locally negligible (10.1.3), it is necessary and sufficient that, for every open set U of X and every differential form of maximum degree ω\omega on U which is locally of integrable modulus, the set A∩UA \cap U be locally negligible for the measure mod(ω)μ\mathrm{mod}(\omega)_\mu.

Suppose in addition that X is paracompact and let ν\nu be a measure on X belonging to the canonical equivalence class M (10.1.4). The measure mod(ω)μ\mathrm{mod}(\omega)_\mu is based on ν\nu (INT, V, § 5, No. 2, def. 2). In order that mod(ω)μ\mathrm{mod}(\omega)_\mu belong to M, it is necessary and sufficient that the set of x∈Xx \in X such that ω(x)=0\omega(x) = 0 be locally negligible.

10.1.7. Example. — Let G be a Lie group over K, of finite dimension nn, and let ω\omega be a differential form of degree nn on G, invariant under left translations, and nonzero. The corresponding measure mod(ω)μ\mathrm{mod}(\omega)_\mu is then a left Haar measure on the locally compact group G.

When G is the multiplicative group K∗K^*, one can take for ω\omega the form dx/xdx/x, and one has mod(ω)μ=(mod)−1.μ\mathrm{mod}(\omega)_\mu = (\mathrm{mod})^{-1}.\mu, cf. INT, VII, § 1, No. 10, prop. 14.

10.2. Orientations

Let us recall that, in this number and the following ones, we suppose that K=RK = \mathbf{R}.

10.2.1 (« Orientation of a real vector space »). Let E be a real vector space of finite dimension nn. We denote by Or(E) the set of orientations of E (A, VI, § 2, No. 7); the elements of Or(E) are the two closed half-lines of the vector space det⁡(E)=⋀nE\det(E) = \bigwedge^n E. If ξ∈Or(E)\xi \in \mathrm{Or}(E), the other element of Or(E) is called the orientation opposite to ξ\xi, and denoted −ξ-\xi.

Let 0→E′→αE→βE′′→00 \to E' \xrightarrow{\alpha} E \xrightarrow{\beta} E'' \to 0 be an exact sequence of (real) vector spaces of finite dimension; put p′=dim⁡E′, p′′=dim⁡E′′p' = \dim E',\ p'' = \dim E'' and let ξ′\xi' (resp. ξ′′\xi'') be an orientation of E' (resp. E''). We denote by ξ′ξ′′\xi'\xi'' (resp. ξ′′ξ′\xi''\xi') the orientation of E containing a (p′+p′′)(p' + p'')-nonzero vector u′∧u′′u' \wedge u'' (resp. u′′∧u′u'' \wedge u'), where u′u' is the image under ∧α\wedge^\alpha of a p′p'-vector of E' belonging to ξ′\xi' and where u′′u'' is a p′′p''-vector of E whose image under ∧β\wedge^\beta belongs to ξ′′\xi'' (cf. A, VI,§ 2, No. 7). If E=E′×E′′E = E' \times E'', α\alpha and β\beta being the canonical mappings, we say that ξ′ξ′′\xi'\xi'' is the product of the orientation ξ′\xi' and of the orientation ξ′′\xi''.

10.2.2 (« Space of orientations »). Let B be a topological space and M a real vector bundle with base B (in the topological sense — cf. § 6, p. 61, Note (*)), of finite rank

(7.1.6). Let OrM\mathrm{Or}_M be the disjoint union of the Or(Mb)\mathrm{Or}(M_b), for b∈Bb \in B, and let π:OrM→B\pi : \mathrm{Or}_M \to B be the mapping such that π(Or(Mb))={b}\pi(\mathrm{Or}(M_b)) = \{b\}. There exists on OrM\mathrm{Or}_M a structure of topological space and only one such that:

a) π\pi is continuous.

b) If ss is a continuous and everywhere nonzero section of det⁡(M)\det(M) on an open set UU of BB, and if ξ(s(b))\xi(s(b)) is the orientation of MbM_b defined by the element s(b)s(b) of det⁡(Mb)\det(M_b), the mapping b↦ξ(s(b))b \mapsto \xi(s(b)) of UU into OrM\mathrm{Or}_M is continuous.

The space OrM\mathrm{Or}_M is called the space of orientations of MM. The group {±1}\{\pm 1\} operates on OrM\mathrm{Or}_M by ξ↦±ξ\xi \mapsto \pm \xi (10.2.1). The quadruplet (OrM,{±1},B,π)(\mathrm{Or}_M, \{\pm 1\}, B, \pi) is a principal fibration (6.2.1) with base BB and structural group {±1}\{\pm 1\}; the projection π:OrM→B\pi : \mathrm{Or}_M \to B defines an isomorphism of OrM/{±1}\mathrm{Or}_M/\{\pm 1\} onto BB, cf. No. 6.2.

When BB is endowed with a structure of variety, OrM\mathrm{Or}_M is endowed with the inverse image structure of that of BB by π\pi (5.8.1); the fibration defined above is then a fibration of varieties and the morphism π\pi is étale.

10.2.3. Retain the hypotheses of 10.2.2. An orientation of the vector bundle MM is called a continuous section ξ:B→OrM\xi : B \to \mathrm{Or}_M of the projection π:OrM→B\pi : \mathrm{Or}_M \to B. We say that MM is orientable if it possesses an orientation; this is equivalent to saying that the bundle OrM\mathrm{Or}_M is trivializable, i.e. isomorphic to B×{±1}B \times \{\pm 1\}. If BB is connected and nonempty, every orientable vector bundle with base BB possesses two orientations, opposite to one another.

When MM is reduced to 0, the bundle det⁡(M)\det(M) is the trivial bundle RBR_B and OrM\mathrm{Or}_M is identified with Or(R)×B\mathrm{Or}(R) \times B; the bundle MM possesses a canonical orientation, corresponding to the positive half-line of RR.

10.2.4 (« Orientation of a variety »). Let XX be a locally finite-dimensional variety over RR of class CrC^r, and let T(X)T(X) be its tangent bundle. We denote by X~\tilde{X} the variety OrT(X)\mathrm{Or}_{T(X)}; the group {±1}\{\pm 1\} operates properly and freely on X~\tilde{X} and X~/{±1}\tilde{X}/\{\pm 1\} is identified with XX; the fibres of the projection π:X~→X\pi : \tilde{X} \to X are the sets Or(Tx(X))\mathrm{Or}(T_x(X)), for x∈Xx \in X. An orientation of XX is called an orientation of the bundle T(X)T(X), in other words a continuous section of the bundle X~\tilde{X}; such a section is of class CrC^r. We say that XX is orientable if it possesses an orientation. Every variety of dimension zero is orientable and possesses a canonical orientation (10.2.3).

Let ξ∈X~\xi \in \tilde{X} and let x=π(ξ)x = \pi(\xi) be its image in XX; the mapping Tξ(π):Tξ(X~)→Tx(X)T_\xi(\pi) : T_\xi(\tilde{X}) \to T_x(X) is an isomorphism; it allows ξ\xi to be identified with an element ξ~\tilde{\xi} of Or(Tξ(X~))\mathrm{Or}(T_\xi(\tilde{X})). The mapping ξ↦ξ~\xi \mapsto \tilde{\xi} is an orientation of X~\tilde{X}, called canonical; in particular, X~\tilde{X} is orientable.

10.2.5 (« Orientation of a morphism »). Let XX and YY be two locally finite-dimensional varieties and let f:X→Yf : X \to Y be a morphism of varieties. An orientation of ff is called a morphism f~:X~→Y~\tilde{f} : \tilde{X} \to \tilde{Y} rendering commutative the diagram

X~→f~Y~∣∣X→fY \begin{array}{ccc} \tilde{X} & \xrightarrow{\tilde{f}} & \tilde{Y} \\ | & & | \\ X & \xrightarrow{f} & Y \end{array}

and compatible with the action of the group {±1}\{\pm 1\}.

If f~\tilde{f} is an orientation of ff and if η\eta is an orientation of YY, there exists one and only one orientation ξ\xi of XX such that the diagram

X~→f~Y~ξ↓η↓X→fY \begin{array}{ccc} \tilde{X} & \xrightarrow{\tilde{f}} & \tilde{Y} \\ \xi \downarrow & & \eta \downarrow \\ X & \xrightarrow{f} & Y \end{array}

is commutative. We say that ξ\xi is associated with η\eta by f~\tilde{f}.

Examples

a) If YY is reduced to a point, an orientation of ff is equivalent to an orientation of XX.

b) Suppose that ff is étale. For every x∈Xx \in X, the mapping Tx(f)T_x(f) is an isomorphism of Tx(X)T_x(X) onto Tf(x)(Y)T_{f(x)}(Y), and defines (by transport of structure) a bijection

f~x:Or(Tx(X))→Or(Tf(x)(Y)). \tilde{f}_x : \mathrm{Or}(T_x(X)) \to \mathrm{Or}(T_{f(x)}(Y)).

The family of the f~x\tilde{f}_x defines an orientation f~:X~→Y~\tilde{f} : \tilde{X} \to \tilde{Y} of ff, called canonical.

c) More generally, suppose that ff is a submersion, and let α\alpha be an orientation of the bundle T(X/Y)T(X/Y) (8.1.3). Let x∈Xx \in X and ξ\xi be an orientation of Tx(X)T_x(X). Put y=f(x)y = f(x); one has an exact sequence (8.1.3)

0→Tx(X/Y)→Tx(X)→Tx(f)Ty(Y)→0 0 \to T_x(X/Y) \to T_x(X) \xrightarrow{T_x(f)} T_y(Y) \to 0

and there exists therefore one and only one orientation f~α(ξ)\tilde{f}_\alpha(\xi) of Ty(Y)T_y(Y) such that ξ=f~α(ξ)α(x)\xi = \tilde{f}_\alpha(\xi)\alpha(x) (10.2.1). The mapping f~α:X~→Y~\tilde{f}_\alpha : \tilde{X} \to \tilde{Y} is an orientation of ff, called associated with α\alpha. The mapping α↦f~α\alpha \mapsto \tilde{f}_\alpha is a bijection of the set of orientations of T(X/Y)T(X/Y) onto the set of orientations of ff.

d) If f:X→Yf : X \to Y is an immersion, the orientations of ff correspond to the orientations of the normal bundle to ff.

10.2.6 (« Orientation of a product »). Let X1X_1 (resp. X2X_2) be a locally finite-dimensional manifold and ξ1\xi_1 (resp. ξ2\xi_2) an orientation of X1X_1 (resp. X2X_2). Let X=X1×X2X = X_1 \times X_2. The mapping (x1,x2)↦ξ1(x1)ξ2(x2)(x_1, x_2) \mapsto \xi_1(x_1)\xi_2(x_2) (10.2.1) is an orientation of X1×X2X_1 \times X_2, called the product of the orientations ξ1\xi_1 and ξ2\xi_2, and denoted by ξ1ξ2\xi_1 \xi_2, or ξ1⊗ξ2\xi_1 \otimes \xi_2.

Suppose that XiX_i (i=1,2i = 1, 2) is purely of dimension nin_i. The canonical isomorphism X1×X2→X2×X1X_1 \times X_2 \to X_2 \times X_1 transforms ξ1⊗ξ2\xi_1 \otimes \xi_2 into ξ2⊗ξ1\xi_2 \otimes \xi_1 (resp. into −ξ2⊗ξ1-\xi_2 \otimes \xi_1) if one of the nin_i is even (resp. if n1n_1 and n2n_2 are odd).

10.2.7 (« Complex case »). Let FF be a finite-dimensional complex vector space and let FRF_\mathbf{R} be the underlying real vector space. Let {e1,…,em}\{e_1, \ldots, e_m\} be a basis of FF; then {e1,ie1,e2,ie2,…,em,iem}\{e_1, ie_1, e_2, ie_2, \ldots, e_m, ie_m\} is a basis of FRF_\mathbf{R} and the orientation of FRF_\mathbf{R} defined by the 2m2m-vector

e1∧ie1∧e2∧ie2∧⋯∧em∧iem e_1 \wedge ie_1 \wedge e_2 \wedge ie_2 \wedge \cdots \wedge e_m \wedge ie_m

is independent of the choice of the basis {e1,…,em}\{e_1, \ldots, e_m\} of FF; this is called the orientation of FRF_\mathbf{R} defined by the given complex structure. If FF is the direct sum of two subspaces GG and HH, the orientation of FR=GR⊕HRF_\mathbf{R} = G_\mathbf{R} \oplus H_\mathbf{R} is the product of the orientations of GRG_\mathbf{R} and HRH_\mathbf{R}.

Let X be a real locally finite-dimensional manifold, endowed with an almost complex structure (8.8.3). For every x∈Xx \in X, let ξ(x)\xi(x) be the orientation of Tx(X)T_x(X) defined by its complex structure. The mapping x↦ξ(x)x \mapsto \xi(x) is an orientation of X, said to be defined by the almost complex structure. In particular, we shall endow the real analytic manifold X underlying a complex analytic manifold XcX^c, locally finite-dimensional, with the orientation defined by the associated almost complex structure (8.8.6). If the given complex analytic manifold structure on X is replaced by its conjugate (5.4.12.b)), this orientation is multiplied by the function x↦(−1)dim⁡RXcx \mapsto (-1)^{\dim_{\mathbf{R}} X^c}.

10.2.8. Examples

a) Let E be a finite-dimensional real vector space. The real analytic manifold defined by E (5.2.2) is orientable. More precisely, the mapping ξ↦ξ(0)\xi \mapsto \xi(0) is a bijection from the set of orientations of this manifold onto Or(E).

In particular, the manifold Rn\mathbf{R}^n has a canonical orientation ξn\xi^n defined by the half-line R+e1∧⋯∧en\mathbf{R}_+ e_1 \wedge \cdots \wedge e_n of Or(Rn\mathbf{R}^n).

(b) Let XX be a sphere with centre 0 and radius >0> 0 in Rn\mathbf{R}^n; it is a submanifold of Rn\mathbf{R}^n. For every x∈Xx \in X, the space Tx(Rn)=RnT_x(\mathbf{R}^n) = \mathbf{R}^n is the direct sum of the right line Rx and the hyperplane Tx(X)T_x(X). Let ηx\eta_x be the orientation R+x\mathbf{R}_+ x of Rx (“outward normal”) and let ξx\xi_x be the unique orientation of Tx(X)T_x(X) such that the product of ηx\eta_x and ξx\xi_x is the orientation ξn\xi^n of Rn\mathbf{R}^n. The mapping x↦ξxx \mapsto \xi_x is an orientation of XX, called canonical.

(c) Let XX be a connected manifold, and let GG be a discrete group acting properly and freely on XX. For X/GX/G to be orientable, it is necessary and sufficient that XX be orientable and that the action of GG on the set of orientations of XX be trivial.

(d) The real projective space Pn−1(R)P_{n-1}(\mathbf{R}) is identified with the quotient of the sphere Sn−1S_{n-1} by the group {±1}\{ \pm 1 \} acting by x↦±xx \mapsto \pm x; it is orientable if nn is even, and non-orientable if nn is odd.

(e) Every quotient of a Lie group by a connected Lie subgroup is orientable.

10.3. M-twisted differential forms

10.3.1. Let XX be a real manifold of class CrC^r, and let MM be a vector bundle with base XX, of finite rank and of class CkC^k, with 0≤k≤r0 \leq k \leq r. Let λM=(OrM,{±1},X,π)\lambda_M = (\mathrm{Or}_M, \{ \pm 1 \}, X, \pi) be the principal fibration associated with the manifold of orientations of MM (10.2.2). Let the structural group {±1}\{ \pm 1 \} act on R\mathbf{R} by multiplication. Denote by R~M\tilde{R}_M the fibre bundle associated with λM\lambda_M with typical fibre R\mathbf{R} (endowed with the law of operation defined above) (6.5.1); it is endowed (7.10.2) with a structure of vector bundle with base XX, of rank 1 and of class CkC^k; it is called the bundle of M-twisted scalars.

10.3.2. We have a commutative diagram:

OrM×R→ρR~M↓pr1↓pOrM→φX \begin{array}{ccc} \mathrm{Or}_M \times \mathbf{R} & \xrightarrow{\rho} & \tilde{R}_M \\ \downarrow \mathrm{pr}_1 & & \downarrow p \\ \mathrm{Or}_M & \xrightarrow{\varphi} & X \end{array}

where pp denotes the canonical projection of R~M\tilde{\mathbf{R}}_M onto XX, ρ\rho the frame mapping (6.5.1) of R~M\tilde{\mathbf{R}}_M and where φ(ξ)=ρ(ξ,1)\varphi(\xi) = \rho(\xi, 1) for ξ∈OrM\xi \in \mathrm{Or}_M. In particular, the inverse image of the bundle R~M\tilde{\mathbf{R}}_M by π\pi is identified with the trivial bundle OrM×R\mathrm{Or}_M \times \mathbf{R}. An element ξ\xi of OrM\mathrm{Or}_M is also identified with its image in R~M\tilde{\mathbf{R}}_M by φ\varphi; with this convention, we have ρ(ξ,a)=aξ\rho(\xi, a) = a\xi for every (ξ,a)∈OrM×R(\xi, a) \in \mathrm{Or}_M \times \mathbf{R}; we have aξ=bηa\xi = b\eta if and only if there exists e∈{±1}e \in \{ \pm 1 \} such that b=eab = ea and η=eξ\eta = e\xi. An orientation ξ\xi of MM thus defines a section x↦ξ(x)x \mapsto \xi(x) of R~M\tilde{\mathbf{R}}_M.

There exists one and only one isomorphism jj of R~M⊗R~M\tilde{\mathbf{R}}_M \otimes \tilde{\mathbf{R}}_M onto the trivial bundle RX=X×RR_X = X \times \mathbf{R} such that j(ξ⊗ξ)=(π(ξ),1)j(\xi \otimes \xi) = (\pi(\xi), 1) for all ξ∈OrM\xi \in \mathrm{Or}_M; this allows the vector bundle R~M\tilde{\mathbf{R}}_M to be identified with its dual.

10.3.3. Let moreover FF be a vector bundle with base XX and of class Cr−1C^{r-1}. A differential form on XX with values in R~M⊗F\tilde{\mathbf{R}}_M \otimes F is called an MM-twisted differential form with values in FF. Such a form of degree pp is a section of the bundle Altp(T(X);R~M⊗F)\mathrm{Alt}^p(T(X); \tilde{\mathbf{R}}_M \otimes F), which is identified in an obvious manner with R~M⊗Altp(T(X);F)\tilde{\mathbf{R}}_M \otimes \mathrm{Alt}^p(T(X); F). When FF is the trivial bundle defined by a Banach space EE, one simply speaks of an MM-twisted form with values in EE; when E=CE = \mathbf{C} (resp. R\mathbf{R}), one says complex MM-twisted form (resp. real MM-twisted form, or MM-twisted form).

Let ω\omega be an MM-twisted form of degree pp with values in FF. The fact that π:OrM→X\pi : \mathrm{Or}_M \to X is étale and that π∗(R~M)=OrM×R\pi^*(\tilde{\mathbf{R}}_M) = \mathrm{Or}_M \times \mathbf{R} allows π∗(RM⊗Altp(T(X);F))\pi^*(\mathbf{R}_M \otimes \mathrm{Alt}^p(T(X); F)) to be identified with Altp(T(OrM);π∗(F))\mathrm{Alt}^p(T(\mathrm{Or}_M); \pi^*(F)) and ω\omega defines a section ω~\tilde{\omega} of Altp(T(OrM);π∗(F))\mathrm{Alt}^p(T(\mathrm{Or}_M); \pi^*(F)) (7.4.3), in other words, a differential form of degree pp on OrM\mathrm{Or}_M with values in π∗(F)\pi^*(F). One thus obtains a bijection from the space of MM-twisted forms of degree pp on XX with values in FF, onto the space of forms ω~\tilde{\omega} of degree pp on OrM\mathrm{Or}_M with values in π∗(F)\pi^*(F) such that

ω~(−ξ)=−ω~(ξ)pour tout ξ∈OrM. \tilde{\omega}(-\xi) = -\tilde{\omega}(\xi) \quad \text{pour tout } \xi \in \mathrm{Or}_M.
When MM is endowed with an orientation ξ\xi, the mapping ω↦ξ⊗ω\omega \mapsto \xi \otimes \omega allows the sections of Altp(T(X);F)\mathrm{Alt}^p(T(X); F) (in other words the usual differential forms of degree pp) to be identified with the MM-twisted forms of degree pp with values in FF.

10.3.4. Let ω\omega be an MM-twisted differential form of degree pp on XX, with values in a Banach space EE, and of class CsC^s (1≤s≤inf⁡(k,r−1)1 \leq s \leq \inf(k, r-1)). There exists one and only one MM-twisted differential form dωd\omega, of degree p+1p+1 on XX, with values in EE, such that, for every open set UU of XX, orientation ξ\xi of M∣UM|U and differential form α\alpha on UU such that ω∣U=ξ⊗α\omega|U = \xi \otimes \alpha, one has dω∣U=ξ⊗dαd\omega|U = \xi \otimes d\alpha. The form dωd\omega is of class Cs−1C^{s-1}; it is called the exterior differential of ω\omega.

If ω~\tilde{\omega} (resp. dω~\tilde{d\omega}) denotes the differential form on OrM\mathrm{Or}_M corresponding to ω\omega (resp. to dωd\omega) as in 10.3.3, one has d(ω~)=dω~d(\tilde{\omega}) = \tilde{d\omega}.

If ζ\zeta is a vector field of class CsC^s on XX, one defines analogously the MM-twisted form θζ.ω\theta_\zeta.\omega. One has

θζ.ω=d(i(ζ)ω)+i(ζ)dω \theta_\zeta.\omega = d(i(\zeta)\omega) + i(\zeta)d\omega
and θζ.ω\theta_\zeta.\omega is of class Cs−1C^{s-1}.

10.4. Measure associated with a twisted differential form

Let us recall that, in this number, we suppose K=RK = \mathbf{R} and that all the varieties considered are locally of finite dimension.

10.4.1. Let X be a variety of class C'. We can apply the definitions and results of 10.3 by taking for vector bundle M the tangent bundle T(X). We then have Or_M = X~\tilde{X} (10.2.4); we denote R~X\tilde{R}_X and simply call the bundle of twisted scalars the bundle R~T(X)\tilde{R}_{T(X)} (10.3.1)[^2]; a T(X)-twisted differential form with values in a vector bundle F is simply called a twisted (or odd) differential form with values in F. When X is endowed with an orientation, the mapping ω↦ξ⊗ω\omega \mapsto \xi \otimes \omega makes it possible to identify the usual differential forms (sometimes called «pairs») with twisted forms.

10.4.2. Let f:X→Yf : X \to Y be a morphism of manifolds of class C' and let f~:X~→Y~\tilde{f} : \tilde{X} \to \tilde{Y} be an orientation of ff (10.2.5). There exists one and only one isomorphism jj of f∗(R~Y)f^*(\tilde{R}_Y) onto R~X\tilde{R}_X such that x~=j(π(x~),f~(x~))\tilde{x} = j(\pi(\tilde{x}), \tilde{f}(\tilde{x})) for every x~∈X~\tilde{x} \in \tilde{X}. We identify these two bundles by means of jj. If ω\omega is a twisted form of degree pp on Y with values in a vector bundle F, the inverse image f∗(ω)f^*(\omega) is identified with a twisted differential form of degree pp on X with values in f∗(F)f^*(F). If we denote by ω~\tilde{\omega} (resp. f~∗(ω)\tilde{f}^*(\omega)) the differential form on Y~\tilde{Y} (resp. X~\tilde{X}) corresponding to ω\omega (resp. f∗(ω)f^*(\omega)) as in 10.3.3, we have f~∗(ω~)=f~∗(ω)\tilde{f}^*(\tilde{\omega}) = \tilde{f}^*(\omega).

When F is the trivial bundle defined by a Banach space, the operation f∗f^* commutes with exterior differentiation (10.3.4).

10.4.3. Let X be a pure manifold of dimension n, and let ω\omega be a twisted differential form of degree n on X, with values in a Banach space E. Let c=(U,φ,Rn)c = (U, \varphi, \mathbf{R}^n) be a chart of X and let ξn\xi^n be the canonical orientation of Rn\mathbf{R}^n; let u1,…,unu^1, \ldots, u^n denote the coordinate functions on Rn\mathbf{R}^n. There exists one and only one function fcf_c on φ(U)\varphi(U), with values in E, such that

ω∣U=φ∗(ξn⊗fc.du1∧⋯∧dun). \omega|U = \varphi^*(\xi^n \otimes f_c . du^1 \wedge \cdots \wedge du^n).

We say that ω\omega is locally integrable if, for every chart c=(U,φ,Rn)c = (U, \varphi, \mathbf{R}^n) of X, the corresponding function fcf_c is locally integrable with respect to λφ(U)⊗n\lambda_{\varphi(U)}^{\otimes n} (where λ\lambda denotes Lebesgue measure on R\mathbf{R}). Suppose that this is the case and that X is separated. There exists on X one and only one vector measure α(ω)\alpha(\omega) with values in E having the following property: for every chart c=(U,φ,Rn)c = (U, \varphi, \mathbf{R}^n) of X, the image by φ\varphi of the restriction to U of the measure α(ω)\alpha(\omega) is the measure fc.λφ(U)⊗nf_c . \lambda_{\varphi(U)}^{\otimes n} (INT, VI, § 2, No. 4). We say that α(ω)\alpha(\omega) is the measure defined by ω\omega and we usually denote it simply by ω\omega. The support of α(ω)\alpha(\omega) is contained in the support Supp ω\omega of ω\omega (where the support of a differential form ω\omega is defined to be the closure of the set of x∈Xx \in X such that ω(x)≠0\omega(x) \neq 0).

If ff is a real function on X, locally integrable with respect to the measure α(ω)\alpha(\omega), then the differential form fωf \omega is locally integrable and we have α(fω)=f.α(ω)\alpha(f \omega) = f . \alpha(\omega).

If gg is a real function on XX essentially integrable for α(ω)\alpha(\omega), its integral is generally denoted ∫Xgω\int_X g \omega, or ∫gω\int g \omega, or ∫g(x)ω(x)\int g(x) \omega(x); one avoids denoting it ∫g dω\int g \, d\omega, because of the risks of confusion with the exterior differential dωd\omega of ω\omega, which is defined (and is moreover equal to 0) if ω\omega is of class C1C^1. If A is a subset of X whose characteristic function φA\varphi_A is essentially integrable for α(ω)\alpha(\omega), the integral of φA\varphi_A is denoted

∫_A ω. If the constant 1 is essentially integrable for α(ω), one says that ω is integrable.

Let now p be an integer, with 0 ≤ p ≤ n, and let ω be a twisted differential form of degree p on X, with values in a Banach space E. Let moreover Y be a pure submanifold of dimension p of X; suppose that the canonical injection i : Y → X is provided with an orientation. The inverse image i*(ω) (10.4.2) is then sometimes denoted ω|Y. If ω|Y is integrable, one sets

∫Yω=∫Yω∣Y. \int_Y \omega = \int_Y \omega|Y.

10.4.4. Let X be a pure manifold of dimension n, provided with an orientation ξ. The identification ω ↦ ξ ⊗ ω between ordinary differential forms and twisted differential forms makes it possible to apply what precedes to forms of degree n on X; thus, to every locally integrable form ω, of degree n, there corresponds a measure on X, again denoted ω. If E = R, such a form ω is locally of integrable modulus (10.1.5) and the corresponding measure mod(ω)_μ (10.1.6) is none other than the absolute value |ω| of the measure ω (INT, III, § 1, No. 6).

10.4.5. Example. — Let X be a pure real manifold of dimension 1, oriented, separated, and let z : X → C be a differentiable mapping of X into C. The complex differential form dz defines on X a complex measure also denoted dz. This applies in particular when X is a pure differential submanifold of dimension 1 of C, z being the injection of X into C.

More particularly, take for X a circle with center 0 and radius ρ > 0; orient X as indicated in 10.2.8, b), taking account of the usual identification of C with R²; if x ∈ X, the tangent space T_x(X) is identified with the right Rix of T_x(C) = C and the chosen orientation is the half-right R_+ ix. If f is a continuous function on X, with values in a complex Banach space, the integral of f for the measure dz is given by the formula

∫Xf(z) dz=iρ∫02πf(ρeiα) eiα dα. \int_X f(z)\,dz = i\rho \int_0^{2\pi} f(\rho e^{i\alpha})\,e^{i\alpha}\,d\alpha.

For example, if n is an integer, we have

∫Xzn dz=iρn+1∫02πe(n+1)iα dα={0if n≠−12iπif n=−1. \int_X z^n\,dz = i\rho^{n+1} \int_0^{2\pi} e^{(n+1)i\alpha}\,d\alpha = \begin{cases} 0 & \text{if } n \neq -1 \\ 2i\pi & \text{if } n = -1. \end{cases}

10.4.6 (« Complex case »). Let X^c be a separated complex analytic manifold, pure of dimension m, and let ω be a holomorphic differential form of degree m on X^c. Let X be the real analytic manifold underlying X^c; the form ω is identified with a form of type (m, 0) on X (8.8.9); let ω‾\overline{\omega} be its conjugate (8.8.2). The form im2ω∧ω‾i^{m^2} \omega \wedge \overline{\omega} is a real differential form of degree 2m on X; taking account of the canonical orientation of X (10.2.7), this form is identified with a measure on X, which is none other than the positive measure mod(ω)_μ defined in 10.1.6, where μ is the measure defined by the differential form i dz∧dzˉi\,dz\wedge d\bar z, in other words twice the Lebesgue measure λ⊗2\lambda^{\otimes 2} on C\mathbf{C} (identified with R2\mathbf{R}^2 in the usual manner).

Let H be the space of holomorphic forms ω\omega of degree m on XcX^c such that the measure ω∧ωˉ\omega\wedge\bar\omega is bounded. For α,β\alpha,\beta in H, the complex measure α∧βˉ\alpha\wedge\bar\beta is bounded; by setting

(α∣β)=im2∫Xα∧βˉ, (\alpha|\beta)=i^{m^2}\int_X \alpha\wedge\bar\beta,

one obtains a Hermitian form on H, which makes H a Hilbert space.

[^1]: When K=RK = \mathbf{R}, it suffices to suppose that r>sup⁡y∈Y(dim⁡f(y)X−dim⁡yY)r > \sup_{y \in Y} (\dim_{f(y)} X - \dim_y Y); cf. for example A. SARD, Bull. Am. Math. Soc., XLVIII (1943), p. 883–890. [^2]: One should take care that this notation is contradictory with the notation R~M\tilde{R}_M when one considers X as provided with its structure of a vector bundle of rank 0 over itself.

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.