Bourbaki

Example

Tag 0EEJ, permanent. Cite it as [Bourbaki, Tag 0EEJ].

Variétés différentielles et analytiques, chapter 2, § 11. Formule de Stokes

When X=RnX = \mathbf{R}^n, ξ\xi is the usual orientation of Rn\mathbf{R}^n and AA is a closed ball of radius >0> 0, the orientation of the sphere ∂A\partial A defined by ξ\xi is the canonical orientation (10.2.8, b)).

11.2.2. Let ω\omega be a twisted differential form of degree pp on XX with values in EE (10.4.1); the inverse image i∗(ω)i^*(\omega) of ω\omega by the oriented morphism i:∂A→Xi : \partial A \to X is denoted by ω∣∂A\omega|_{\partial A} and is called the form induced by ω\omega on ∂A\partial A (cf. 10.4.3).

11.2.3. Let us make one of the following two hypotheses:

(i) ω\omega is a twisted differential form of degree n−1n-1 on XX, with values in EE; (ii) XX is oriented, ∂A\partial A is provided with the corresponding orientation (11.2.1) and ω\omega is a differential form of degree n−1n-1 on XX with values in EE.

Suppose in addition that ω\omega is of class C1C^1 and that the intersection of AA and the support of ω\omega is compact. The exterior differential dωd\omega of ω\omega is continuous (8.3.5 and 10.3.4).

The characteristic function of AA is essentially integrable for the vector measure defined by dωd\omega on XX and the differential form ω∣∂A\omega|_{\partial A} of degree n−1n - 1 on ∂A\partial A is integrable (10.4.3 and 10.4.4). One has

∫Adω=∫∂Aω(« Stokes formula »). \int_A d\omega = \int_{\partial A} \omega \quad \text{(« Stokes formula »)}.
11.2.4. Let α\alpha be a twisted differential form of degree nn on XX with values in EE, with compact support, and of class C1C^1. In order that there exist a twisted differential form ω\omega of degree n−1n - 1 on XX, with values in EE, with compact support and of class C1C^1, such that α=dω\alpha = d\omega, it is necessary that ∫Xα=0\int_X \alpha = 0; if XX is connected, this condition is sufficient; if in addition α\alpha is of class CkC^k (k≤r−1,k≠ωk \leq r - 1, k \neq \omega), one can choose ω\omega of class CkC^k.

11.2.5. Suppose that XX is the real variety underlying C\mathbf{C}, that EE is a complex Banach space and that AA is a compact piece of XX. Equip XX with the orientation defined by its complex structure (10.2.7). Let ff be a continuous mapping from AA into EE whose restriction to the interior A˚\mathring{A} of AA is holomorphic. Let dzdz denote the differential of the injection z:∂A→Cz : \partial A \to \mathbf{C}. The form f.dzf.dz, product of ff and dzdz, is a differential form of degree 1 on ∂A\partial A, with values in EE, of class C0C^0, and one has:

∫∂Af.dz=0(« Cauchy formula »). \int_{\partial A} f.dz = 0 \quad \text{(« Cauchy formula »)}.
When ff extends to a holomorphic mapping, still denoted ff, of an open neighbourhood UU of AA, with values in EE, the differential form f.dzf.dz (where zz denotes this time the canonical injection of UU into C\mathbf{C}) is of class C∞C^\infty on UU and its exterior differential is zero.

11.2.6 (Derivative of an integral). Suppose XX is oriented. Let YY be a variety of class CrC^r, and let α\alpha be a differential form of degree nn on YY, with values in EE, of class C1C^1, and with compact support. Let II be an open subset of R\mathbf{R} containing 0 and let g:I×X→Yg : I \times X \to Y be a morphism of class CrC^r; for t∈It \in I, denote by gtg_t the mapping x↦g(t,x)x \mapsto g(t, x) from XX into YY. Denote by ψ\psi the morphism from XX into T(Y)T(Y) defined by ψ(x)=T(0,x)(g)(1,0)\psi(x) = T_{(0, x)}(g)(1, 0); it is a lifting of g0g_0 (8.6.5). Suppose that the restriction of pr1:I×A→I\mathrm{pr}_1 : I \times A \to I to the intersection of I×AI \times A and the support of g∗(α)g^*(\alpha) is proper (TG, I, § 10). For every t∈It \in I, the intersection of AA and the support of gt∗(α)g_t^*(\alpha) is then compact; the mapping t↦∫Agt∗(α)t \mapsto \int_A g_t^*(\alpha) is of class C1C^1 on II and its derivative at the origin is given by the formula

ddt(∫Agt∗(α))t=0=∫Aθψ⋅α=∫Ai(ψ) dα+∫∂Ai(ψ) α, \frac{d}{dt} \left( \int_A g_t^*(\alpha) \right)_{t=0} = \int_A \theta_\psi \cdot \alpha = \int_A i(\psi) \, d\alpha + \int_{\partial A} i(\psi) \, \alpha,
cf. No. 8.6.

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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