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FALSE: every L2 field on T3 has absolutely convergent Fourier coefficients. An explicit H0 family with ∑k∣u^(k)∣=∞

Statement refuted

False statement. Every field u∈H0(T3;R3)=L2(T3;R3) has absolutely convergent Fourier coefficients: ∑k∈Z3∣u^(k)∣2<+∞. (By Sobolev embedding on the torus: Hσ⊆Cj for σ>j+3/2, with continuous representatives the corresponding statement for Hσ with σ>3/2 is true; the false statement drops the hypothesis, and that is exactly what fails.)

Facts & Assumptions

Given: The weights wk, the shell decomposition {∣k∣∞=L} for L∈N, and the coefficient family u^.

[F1]

If f:[0,∞)→R is nonincreasing and nonnegative, then ∑k≥0f(k) converges if and only if the integrals ∫0Nf are bounded (The integral test: for f≥0 nonincreasing on [0,∞), ∑kf(k) converges if and only if the sequence (∫0Nf)N is bounded, with ∫0Nf≤∑k<Nf(k)≤f(0)+∫0Nf); in particular ∑L≥2L−1(log⁡L)−2<∞ and ∑L≥2L1/2(log⁡L)−1=+∞.

[F2]

A nonnegative extended sum over an index set is the supremum of its finite partial sums, and it is finite exactly when those partial sums are bounded (Series in the nonnegative extended real line).

[F3]

The Fourier coefficient map is a bijection from the real classes of L2(T3;R3) onto the real-symmetric families in ℓ2(Z3;C3), and ∥u∥L22=∑k∣u^(k)∣22 (The Fourier basis and Parseval's identity on the finite torus, Periodic vector Sobolev spaces on the three-torus, the weight family, and the Leray projection).

[F4]

The statement refuted would, if true, force ∑k∣u^(k)∣2<∞ for every real-symmetric square-summable family (Sobolev embedding on the torus: Hσ⊆Cj for σ>j+3/2, with continuous representatives records the correct positive result under σ>3/2).

Counterexample

Use the conventions of Periodic vector Sobolev spaces on the three-torus, the weight family, and the Leray projection: wk=(1+4π2∣k∣22)1/2 and ∥u∥H02=∑k∣u^(k)∣22. Let v:=13(1,1,1)∈R3 and define the real vector field u by the coefficient family u^(k):={0,∣k∣∞≤1,wk−3/2log⁡wk v,∣k∣∞≥2. The family is real-symmetric (u^(−k)=u^(k)=u^(k)‾), so it defines a real field u∈H0. Then ∥u∥H02<+∞ while ∑k∣u^(k)∣2=+∞: the coefficient series of this L2 field is not absolutely convergent.

Proof technique: direct; count the shells ∣k∣∞=L, compare the two series with the integral test, and invoke the Fourier coefficient isometry.

Given: The coefficient family u^ and the facts [F1]-[F4].

1.1givenalgebra

For ∣k∣∞=L the weight satisfies 2πL≤wk≤cL with c:=1+12π2, and the shell has exactly (2L+1)3−(2L−1)3=24L2+2 points. Hence for L≥2, with ℓL:=log⁡(2πL) one has two-sided bounds c−3/2L−3/2/log⁡(cL)≤∣u^(k)∣2≤(2πL)−3/2/ℓL on that shell, so shell summation (multiplicity 24L2+2) gives c1∑L≥2L1/2/log⁡L≤∑k∣u^(k)∣2≤c2∑L≥2L1/2/log⁡L and c3∑L≥21/(Llog⁡2L)≤∑k∣u^(k)∣22≤c4∑L≥21/(Llog⁡2L) for positive constants ci.

2.1step 1.1F1F2

By [F1] the series ∑L≥21/(Llog⁡2L) converges (its integral test function t−1(log⁡t)−2 has finite integral from 2 to ∞, the antiderivative being −1/log⁡t) while ∑L≥2L1/2/log⁡L diverges (its summands do not tend to 0); by [F2] this means ∥u∥H02=∑k∣u^(k)∣22<+∞ and ∑k∣u^(k)∣2=+∞.

3.1step 2.1F3F4∎

The family is real-symmetric by construction, so by [F3] it is the coefficient family of a real field u∈H0; by step 2.1 the hypothesis of the false statement is satisfied but its conclusion fails. Hence the false statement is refuted.

Remarks

  • The counterexample isolates the exact role of the hypothesis σ>3/2 in Sobolev embedding on the torus: Hσ⊆Cj for σ>j+3/2, with continuous representatives: the proof there bounds ∑∣u^(k)∣ by the Cauchy-Schwarz factor (∑kwk−2σ)1/2, which is finite precisely when 2σ>3. At σ=0 this mechanism is unavailable and, as shown, the conclusion is false.
  • Nothing is asserted here about the continuity of this particular field; the refuted statement concerns absolute convergence of its Fourier coefficients only, and the witness is a coefficient family in H0.

Depends on

Dependency tree · 2 levels

Sources