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LemmaStatement: AI-adaptedProof: AI-adaptedPipeline-generatedjudge pass (gpt-6.1-sol)
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Localization: vanishing integrals or fluxes force a continuous function to vanish

Statement

Assume the Axiom of Countable Choice (ACω, The Axiom of Countable Choice (ACω)).

Integral form. Let n,m≥1, let U⊆Rn be open, and let g:U→Rm be continuous. Write gi(x):=g(x)(i) for 0≤i<m, using the canonical function coordinates of The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn. For a measurable V⊆U write, componentwise,

∫Vg dλn:=(∫g0χV dλn, …, ∫gm−1χV dλn),

each component 0≤i<m, when integrable, being the Lebesgue integral of gi on V, extended by zero outside V (Integrable real and complex functions, and their integrals, Integral over a measurable subset). A ball V⊆U is compactly contained in U when its closure is a compact subset of U; for a Euclidean ball this means V‾⊆U. If ∫Vg dλn=0 for every ball V compactly contained in U, then g=0 on U.

Disc form. Let W⊆R3 be open and let F:W→R3 be continuous. Write Fi(x):=F(x)(i) for 0≤i<3 and e0=(1,0,0), e1=(0,1,0), e2=(0,0,1), the canonical standard vectors of The standard list e:n→Fn with ei(i)=1F and ei(j)=0F for j≠i is an ordered basis of Fn; hence dim⁡FFn=n, and F0 is the zero space with basis ∅ and dimension 0. Extend the basis labels cyclically by ej:=ej mod 3 for j≥3. Thus ei+1×ei+2=ei for each i∈{0,1,2}. For such i, q∈W and r>0 put

φi,q(s,t):=q+s ei+1+t ei+2,Dr:={(s,t)∈R2:s2+t2<r2},

with Dr‾ the closed disc. If for every i, every q∈W and every r>0 with φi,q(Dr‾)⊆W one has

∫Dr‾(Fi∘φi,q) dλ2=0,

then F=0 on W.

Conventions. The displayed disc condition is the vanishing of the flux of F through the flat disc φi,q(Dr‾) in the orientation with unit normal ei: the affine parametrization is a regular patch whose tangent vectors ei+1,ei+2 have cross product ei of norm one (Regular parametrized surface patches on compact Jordan parameter regions, The cross product in R3, The standard list e:n→Fn with ei(i)=1F and ei(j)=0F for j≠i is an ordered basis of Fn; hence dim⁡FFn=n, and F0 is the zero space with basis ∅ and dimension 0), so the flux of Unit normal fields, orientations, and flux through a regular surface patch is the Riemann integral ∫Dr‾(Fi∘φi,q) d(s,t); that integral equals the displayed Lebesgue integral because the integrand is continuous on the compact Jordan region Dr‾ (A closed disc of radius r≥0 has Jordan content πr2, The Riemann integral of a bounded function over a bounded Jordan measurable set, A continuous real function on a compact Jordan measurable set is Riemann integrable over that set, Borel Darboux integrands in finite dimension). Both clauses are pointwise conclusions on their open domains. The first clause is the converse from universal integral relations to a pointwise equation; a single vanishing integral over one ball or one disc supplies no conclusion, and the hypothesis ranges over the full family described.

Facts & Assumptions

Given: The Axiom of Countable Choice; integers n,m≥1; an open U⊆Rn and a continuous g:U→Rm with ∫Vg dλn=0 for every ball V compactly contained in U; an open W⊆R3 and a continuous F:W→R3 satisfying the disc condition of the Statement, with canonical indices 0≤i<m for gi and 0≤i<3 for Fi,ei; and, inside the contradiction argument below, either a point p∈U with g(p)≠0 or a point x∈W with F(x)≠0.

[F1]

Metric balls and continuity at a point: BX(a,ρ)={y∈X:dX(y,a)<ρ}, and f is continuous at a when for every real ε>0 there is δ>0 with f[BX(a,δ)]⊆BY(f(a),ε) (Open ball, closed ball and sphere in a metric space, Continuity of a map between metric spaces, at a point and globally, in the ε-δ form).

[F2]

Open subsets of a metric space: U is open exactly when every x∈U has r>0 with B(x,r)⊆U (The metric topology: a set is open when every one of its points has a ball around it inside the set; closed means open complement).

[F3]

Under ACω, every Euclidean ball B(x,r) with r>0 is Lebesgue measurable with 0<λ(B(x,r))<∞ (Euclidean balls have positive finite Lebesgue measure).

[F4]

Integral of signed and nonnegative functions: for measurable real u with at most one of ∫u+, ∫u− equal to +∞ one sets ∫u dλ:=∫u+dλ−∫u−dλ, and u is integrable when both are finite, equivalently ∫∣u∣ dλ<∞; then ∫(−u) dλ=−∫u dλ; and for nonnegative measurable f the integral over E is ∫Ef dλ=∫fχE dλ (Integrable real and complex functions, and their integrals, Integral over a measurable subset).

[F5]

Monotonicity and nonnegative homogeneity for the nonnegative integral: if 0≤f≤h are measurable then ∫f dλ≤∫h dλ, and if c>0 then ∫cf dλ=c∫f dλ (Monotonicity and nonnegative homogeneity of the nonnegative integral).

[F6]

Simple integral: for a nonnegative simple measurable function s=∑j≤NcjχEj one has ∫s dλ=∑j≤Ncjλ(Ej) with 0⋅∞=0, and the nonnegative integral of a nonnegative simple measurable function equals its simple integral; hence ∫cχE dλ=cλ(E) for c≥0 and measurable E (The integral of a nonnegative simple function, The nonnegative integral agrees with the simple integral on simple functions).

[F7]

Measurability: every continuous map Rn→Rm is Borel measurable under ACω; the Borel σ-algebra is generated by the open sets, so indicators of open sets are Borel (Continuous functions on Euclidean spaces are Borel measurable, The Borel sigma-algebra of a topological space).

[F9]

Canonical coordinates: Rm consists of functions on m={0,…,m−1}, zi=z(i) for i<m, and ⟨z,w⟩=∑i<mziwi with ∥z∥2=⟨z,z⟩ (The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn). The standard vectors ei, i<m, have coordinate 1 at i and 0 at the other coordinates (The standard list e:n→Fn with ei(i)=1F and ei(j)=0F for j≠i is an ordered basis of Fn; hence dim⁡FFn=n, and F0 is the zero space with basis ∅ and dimension 0). Hence ∣zi∣≤∥z∥2, since zi2≤∑k<mzk2, and ⟨z,ei⟩=zi; applying the bound to differences shows that every component of a continuous vector map is continuous.

Proof

technique · contradiction; assume the Statement fails, and contradict in turn a nonzero value of $g$ (cases (A)) and, under the disc hypothesis, a nonzero value of $F$ (case (B))
1.1givenassume-contra

Suppose the Statement fails. Then either (A) g(p)≠0 for some p∈U, or (B) the disc condition holds and F(x)≠0 for some x∈W; if neither holds then g=0 on U and, whenever the disc condition holds, F=0 on W, which is exactly the Statement. We contradict (A) and (B) in turn.

2.1step 1.1F1F2F4F9givenalgebra

In case (A): choose a component index i<m with gi(p)≠0 and put u:=gi, continuous by [F9]. Replacing the i-th component of g by its negative preserves the hypothesis, since ∫V(−gi) dλ=−∫Vgi dλ by [F4], and does not change whether g vanishes; hence we may suppose u(p)=2c with c:=u(p)/2>0. By [F1] applied to the continuous u at p with ε=c there is δ0>0 with ∣u(y)−u(p)∣<c for all y∈B(p,δ0); by [F2] and p∈U there is δ2>0 with B(p,δ2)⊆U; put δ:=min⁡{δ0,δ2}>0. Then the ball V:=B(p,δ/2) satisfies V‾⊆B(p,δ)⊆U, so V is compactly contained in U, and u(y)>u(p)−c=c for every y∈V. The hypothesis gives ∫Vg dλn=0, whose i-th component is ∫uχV dλ=0.

2.2step 1.1F1F2F9givenalgebra

In case (B): choose i∈{0,1,2} with Fi(x)≠0 and put φ:=φi,x, W′:=φ−1[W]={(s,t):φ(s,t)∈W} and h:=Fi∘φ:W′→R, so that h(0,0)=Fi(x)≠0. Then W′ is open in R2, h is continuous, and for every r>0 with B‾((0,0),r)⊆W′ the disc hypothesis with centre x gives ∫B‾((0,0),r)h dλ2=0. Indeed, the standard unit vectors are orthonormal by [F9], so ∥φ(s,t)−φ(s′,t′)∥2=∥(s,t)−(s′,t′)∥2 for all (s,t),(s′,t′); hence φ is continuous, and the inverse image of a ball contained in W at φ(s0,t0) contains the parameter ball of the same radius at (s0,t0), so W′ is open by [F2], while for (s0,t0)∈W′ and ε>0, continuity of Fi by [F9] at φ(s0,t0)∈W gives ρ>0 with ∣Fi(y)−Fi(φ(s0,t0))∣<ε whenever d(y,φ(s0,t0))<ρ, and then d((s,t),(s0,t0))<ρ gives ∣h(s,t)−h(s0,t0)∣<ε by the isometry identity; finally, when B‾((0,0),r)⊆W′ the disc φ(B‾((0,0),r)) lies in W, so the Statement's condition applies with centre x and radius r.

3.1step 2.1F3F4F5F6F7F8algebra

In case (A): the function uχV is Borel and nonnegative, and 0≤cχV≤uχV pointwise, because u>c>0 on V by step 2.1 while uχV=0 off V, and u is continuous while V is open [F7]. More explicitly, for a continuous function on open U, inverse images of open real sets are relatively open, hence open in Rn; after multiplication by χV and zero extension, inverse images are Borel (adding Rn∖V when the target contains zero). Moreover V‾ is a nonempty compact metric space, so M:=max⁡V‾∣u∣ is finite by [F8], and ∣uχV∣≤MχB(p,δ) with ∫MχB(p,δ) dλ=Mλ(B(p,δ))<∞ by [F5], [F6] and [F3]; hence uχV is integrable and ∫uχV dλ is a finite real number by [F4]. Monotonicity [F5] and the simple-integral rule [F6] give ∫uχV dλ≥∫cχV dλ=c λ(V)>0 by [F3], contradicting ∫uχV dλ=0 from step 2.1. Therefore case (A) is impossible: the integral hypothesis forces g=0 on U.

4.1step 2.1step 2.2step 3.1F3F4F5F6F8algebra

In case (B), replace h by −h if necessary, which preserves every zero disc integral by [F4], so h(0,0)=2c′>0. Continuity and openness as in step 2.1 give r>0 with B‾((0,0),r)⊆W′ and h>c′ throughout that closed disc C. It is compact by [F8] and contained in the open ball B((0,0),2r), of finite measure by [F3], so hχC is integrable by the boundedness and Borel argument of step 3.1. Since 0≤c′χB((0,0),r)≤hχC, [F5] and [F6] give ∫Ch dλ2≥c′λ2(B((0,0),r))>0 by [F3]. This contradicts the closed-disc integral hypothesis of step 2.2, without replacing it by an unstated open-ball hypothesis. Thus F=0 on W.

5.1step 3.1step 4.1discharge-contradiction∎

Cases (A) and (B) both end in contradiction, so no failure of the Statement occurs: the integral hypothesis forces g=0 on U, and the disc hypothesis forces F=0 on W.

Remarks

  • The proof uses, for each clause, the hypothesis only on balls centred at the point where the function is assumed nonzero and with radius half of a continuity threshold; the full family in the Statement is what makes the lemma a localization statement, but no choice from the family is made, and the argument is choice-free apart from the declared ACω used by the surface and measurability suppliers.
  • The disc clause is not a statement about a single loop or box: one special disc carries no information, and the components must be tested in all three coordinate directions at all admissible centres and radii.

Depends on

Dependency tree · 2 levels

Sources