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The fundamental lemma of the calculus of variations for continuous coefficients

Statement

Assume the Axiom of Countable Choice (ACω). Let n,m≥1, let U⊆Rn be open, and let g:U→Rm be continuous. If ∫U⟨g,h⟩ dλ=0 for every h∈Cc∞(U;Rm), then g=0 on U. Here ⟨⋅,⋅⟩ is the Euclidean inner product and ∫U⟨g,h⟩ dλ is the finite sum ∑i<m∫Ugihi dλ of integrals of continuous compactly supported functions (Integral over a measurable subset). The scalar case is m=1: a continuous g with ∫Ugh dλ=0 for every h∈Cc∞(U;R) vanishes on U. The vector case is deduced from the scalar case componentwise, each component tested separately. The conclusion is pointwise on U, and the hypothesis is the full family of compactly supported smooth test functions. The Axiom of Countable Choice is declared because the localization lemma Localization: vanishing integrals or fluxes force a continuous function to vanish and the measurability fact Continuous functions on Euclidean spaces are Borel measurable used in the recorded proof assume it; no other choice principle enters.

Conventions. Cc∞(U;Rm) is the space of smooth Rm-valued functions with compact support in U, defined componentwise in the sense of Ck Euclidean maps and diffeomorphisms and Test function space d of an open set. Each product gihi is continuous on U and vanishes outside a compact subset of U, and ∫Ugihi dλ denotes the Lebesgue integral of its zero extension to Rn, where λ=λn is n-dimensional Lebesgue measure (Integrable real and complex functions, and their integrals); [F5] and [F6] below record that this is a finite real number and that for a nonnegative integrand it agrees with the nonnegative integral over the measurable set U of Integral over a measurable subset.

Facts & Assumptions

Given: The Axiom of Countable Choice ACω; naturals n,m≥1; an open set U⊆Rn; a continuous g:U→Rm with ∫U⟨g,h⟩ dλ=0 for every h∈Cc∞(U;Rm); and, inside the contradiction argument below, a point p∈U with g(p)≠0.

[F1]

Cutoff lemma, in ZF: for a compact set K⊆Ω with Ω⊆Rn open there is χ∈Cc∞(Ω) with 0≤χ≤1 and χ=1 on a neighborhood of K (Test function cutoffs and euclidean localization).

[F2]

Localization, under ACω: if G:U→Rm is continuous on an open set U and ∫VG dλn=0 for every ball V compactly contained in U, then G=0 on U (Localization: vanishing integrals or fluxes force a continuous function to vanish, where ∫VG is the componentwise integral over the measurable set V). Below we use only its contrapositive form: if G(q)≠0 for some q∈U, then some ball V compactly contained in U has ∫VG dλn≠0.

[F3]

Order and scalar rules for the nonnegative integral (Monotonicity and nonnegative homogeneity of the nonnegative integral): for nonnegative measurable f≤h one has ∫f dλ≤∫h dλ, and for c>0 one has ∫cf dλ=c∫f dλ, while the zero function has integral 0; the nonnegative integral over a measurable set of Integral over a measurable subset is an instance of this integral.

[F4]

Continuity of pairings: if f,w:U→Rm are continuous then x↦⟨f(x),w(x)⟩ is continuous (A vector-valued function has a limit, or is continuous, if and only if each of its components does; with the algebra of continuous vector-valued functions, clause 3); for m=1 this is the ordinary product of two continuous real functions under The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn. In particular the components gi of g are continuous, and for ψ∈Cc∞(U;R) the function ψei lies in Cc∞(U;Rm) and has ⟨g,ψei⟩=giψ.

[F5]

Signed integral (Integrable real and complex functions, and their integrals): for measurable real F with at most one of ∫F+ dλ, ∫F− dλ equal to +∞, one sets ∫F dλ:=∫F+ dλ−∫F− dλ; F is integrable when both parts are finite. If F≥0 then F−=0 and the signed integral of F equals its nonnegative integral, which over a measurable set E is the integral of FχE (Integral over a measurable subset); and ∫(−F) dλ=−∫F dλ is definitional from (−F)+=F− and (−F)−=F+.

[F6]

Compactly supported continuous functions have finite integrals: let F:Rn→R be continuous with compact support K. If K=∅ then F=0 and ∫F dλ=0; otherwise K is a nonempty compact metric space, so M:=max⁡K∣F∣ is finite (A continuous real-valued function on a nonempty compact metric space is bounded and attains a greatest and a least value), K is bounded (A compact subset of a metric space is closed and bounded) hence contained in a closed box Q with λ(Q)<+∞ (A box in Rn with parameters ai≤bi is Lebesgue measurable of measure ∏i<n(bi−ai), whichever of its faces are included), F is Borel measurable (Continuous functions on Euclidean spaces are Borel measurable, under ACω), and ∣F∣≤MχQ, so ∫∣F∣ dλ≤∫MχQ dλ=Mλ(Q)<+∞ by Monotonicity and nonnegative homogeneity of the nonnegative integral, The nonnegative integral agrees with the simple integral on simple functions and The integral of a nonnegative simple function; thus F is integrable by [F5]. In particular each integrand gihi of the hypothesis has a continuous compactly supported zero extension by [F4], and each pairing in the hypothesis is a finite real number.

[F7]

Continuity in balls (Continuity of a map between metric spaces, at a point and globally, in the ε-δ form, Open ball, closed ball and sphere in a metric space): u is continuous at p when for every real ε>0 there is δ>0 with u[B(p,δ)]⊆B(u(p),ε); and B(p,δ)={x:d(p,x)<δ} for δ>0.

Proof

technique · contradiction; assume a point where $g\ne0$, reduce to a scalar continuous function with a vanishing test pairing, and construct a nonnegative compactly supported product of that coefficient with an admissible smooth test function, whose integral is both $0$ and positive
1.1givenF4F5assume-contra

Suppose the conclusion fails: g(p)≠0 for some p∈U. If m=1, put u:=g; then u is continuous and the hypothesis reads ∫Uuψ dλ=0 for every ψ∈Cc∞(U;R). If m≥2, choose i<m with gi(p)≠0 and put u:=gi; for every ψ∈Cc∞(U;R) the function ψei lies in Cc∞(U;Rm) with ⟨g,ψei⟩=giψ by [F4], so the hypothesis gives ∫Uuψ dλ=0. In both cases u:U→R is continuous with u(p)≠0, and replacing u by −u preserves the vanishing pairing because ∫U(−u)ψ dλ=−∫Uuψ dλ by [F5]; hence we may assume u(p)>0.

2.1step 1.1F7algebra

Continuity of u at p with u(p)>0 yields δ>0 with B(p,δ)⊆U and u(x)≥u(p)/2 for every x∈B(p,δ): taking ε:=u(p)/2>0 in [F7] gives δ0>0 with ∣u(x)−u(p)∣<u(p)/2 for d(p,x)<δ0, and since U is open one may shrink δ0 to a δ>0 with B(p,δ)⊆U, the bound remaining valid on the smaller ball.

3.1step 2.1F1

Apply [F1] with Ω:=B(p,δ) and K:={p}: there is χ∈Cc∞(B(p,δ)) with 0≤χ≤1 and χ=1 on a neighborhood of p. Extended by zero, χ lies in Cc∞(U;R) and satisfies supp⁡χ⊆B(p,δ).

4.1step 2.1step 3.1F1F4algebra

Put φ:=uχ, extended by zero to Rn. Then φ is continuous and compactly supported in U by [F4] and [F1], satisfies φ≥0 on U because φ=0 where χ=0 and φ(x)=u(x)χ(x)≥(u(p)/2)χ(x)≥0 for x∈B(p,δ) by step 2.1, and has φ(p)=u(p)>0; hence φ is not the zero function.

5.1step 3.1step 4.1givenF5F6

The hypothesis at the admissible test function χ gives ∫Uuχ dλ=0, that is ∫Uφ dλ=0: since φ≥0, the signed integral equals the nonnegative integral of φ over the measurable set U by [F5], and that integral is a finite real number by [F6].

5.2step 4.1F2F3

By the contrapositive localization [F2] applied to the continuous function φ with φ(p)≠0, there is a ball V compactly contained in U with ∫Vφ dλ≠0; as φ≥0, monotonicity in [F3] applied to the zero function below φχV gives ∫Vφ dλ≥0, so this integral is strictly positive.

6.1step 5.1step 5.2F3discharge-contradiction∎

Since V⊆U, the nonnegative measurable functions φχV and φχU satisfy φχV≤φχU pointwise, so monotonicity in [F3] gives ∫Vφ dλ≤∫Uφ dλ=0, contradicting step 5.2; therefore no point p∈U with g(p)≠0 exists and g=0 on U.

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