Alphabeta Math
LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedprecheck passjudge pass (gpt-6.1-sol)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Band-limited samples are the Fourier coefficients of the rescaled spectrum

Statement

Assume Countable Choice (The Axiom of Countable Choice (ACω)). Let h>0 and let f∈L2(R;C) have Plancherel transform f^:=F2f (Plancherel theorem) vanishing almost everywhere off the band [−1/(2h),1/(2h)]. Then f^∈L1, so f has a continuous representative, again written f, with f(x)=∫Rf^(ξ)e2πixξ dξ for every x. Choose a measurable representative of f^, set Gh(θ):=h−1/2f^(−θ/h) on the half-open interval [−1/2,1/2), and extend Gh one-periodically to R. Its almost-everywhere class is independent of the chosen representative and defines a function class on the circle T=R/Z (The one-dimensional torus and its normalized Haar integral). Then Gh∈L2(T;C), and for every k∈Z its k-th Fourier coefficient (Fourier coefficients and trigonometric polynomials on the torus) is Gh^(k)=h1/2f(hk). Consequently (h1/2f(hk))k∈Z∈ℓ2(Z) and ∑k∈Z∣f(hk)∣2=h−1∥f∥L2(R)2. The reflection θ↦−θ in the definition of Gh is inserted only so that the library's negative-sign coefficient convention matches the samples f(hk) rather than f(−hk).

Facts & Assumptions

[F1]

Plancherel: Fourier transformation on Schwartz space extends uniquely to a surjective complex-linear isometry F2:L2(R;C)→L2(R;C) preserving inner products (Plancherel theorem).

[F2]

Inversion: F22f=Rf with Rf(x)=f(−x), and F2−1=RF2 (L2 Fourier inversion).

[F3]

Agreement: if g∈L1∩L2, its bounded continuous integral transform g^(ξ)=∫g(x)e−2πixξ dx represents F2g almost everywhere (Agreement of the integral and L2 transforms).

[F4]

The integral transform maps L1(R;C) complex-linearly into the bounded uniformly continuous functions, with sup⁡ξ∣g^(ξ)∣≤∥g∥1 (The L1 transform is bounded and uniformly continuous).

[F5]

Finite-measure inclusion: on a measure space of finite measure, Lr⊆Lp for 1≤p<r<∞ with ∥g∥p≤μ(X)1/p−1/r∥g∥r (Finite-measure Lr includes into Lp for p<r).

[F6]

C1 change of variables for L1 functions on open subsets of R (A C^1 diffeomorphism satisfies the change-of-variables formula for L^1 functions).

[F7]

Riesz–Fischer: the Fourier coefficient map Φ:L2(T;C)→ℓ2(Z;C) is a surjective linear isometry, so ∑k∣G^(k)∣2=∥G∥L2(T)2 (Riesz–Fischer: the Fourier coefficient map is onto the space of square-summable families).

[F8]

The torus integral is integration of the representative on [0,1) against λ1, and G^(k)=∫TG e−k dmT with e−k(θ)=e−2πikθ (The one-dimensional torus and its normalized Haar integral, Fourier coefficients and trigonometric polynomials on the torus).

Given: Countable Choice, h>0, a class f∈L2(R;C) with f^=F2f vanishing almost everywhere off B:=[−1/(2h),1/(2h)], and the L2 classes of The space Lp(μ) as the quotient by null functions.

Proof

1.1F5F9givenalgebra

The class f^ is represented by f^1B, which lies in L2(B) with the same norm, and B has finite Lebesgue measure 1/h by [F9]. Applying [F5] on B with p=1, r=2 gives f^∈L1(R;C) with ∥f^∥1≤(1/h)1/2∥f^∥2.

2.1F1F2F3F4step 1.1algebra

Define H(x):=∫Rf^(ξ)e2πixξ dξ for x∈R. Since ξ↦f^(ξ)e2πixξ has modulus ∣f^∣∈L1 by step 1.1, the integral converges absolutely, and x↦H(x)=g^(−x) with g:=f^∈L1∩L2; hence H is bounded and continuous by [F4] and reflection. By [F3], g's integral transform represents F2g=F2f^=Rf almost everywhere by [F2], so H represents R(Rf)=f almost everywhere. Replacing the class f by its continuous representative H gives f(x)=∫Rf^(ξ)e2πixξ dξ for every x, and this replacement changes no L2 class.

3.1F1F6F8F9step 2.1algebra

Represent Gh on the fundamental interval [0,1) by Gh(θ)=h−1/2f^(−θ~/h), where θ~ is the unique representative of θ+Z in [−1/2,1/2). Substituting ξ=−θ/h on (0,1/2) and ξ=(1−θ)/h on (1/2,1), and integrating ∣Gh∣2 with [F6], the factor h−1 from ∣Gh∣2 cancels the Jacobian h, giving ∫T∣Gh∣2 dmT=∫−1/(2h)1/(2h)∣f^(ξ)∣2 dξ=∥f^∥22=∥f∥22, so Gh∈L2(T;C). The endpoints are null, and the same substitutions show that changing the spectrum on a null set changes Gh only on a null set. The same two substitutions applied to Ghe−k, using e−2πik(1−hξ)=e2πikhξ on the right piece, supply the Jacobian h to the prefactor h−1/2 and give Gh^(k)=h1/2∫−1/(2h)1/(2h)f^(ξ)e2πikhξ dξ=h1/2f(hk), the last equality being step 2.1 evaluated at x=hk.

4.1F7step 3.1algebra∎

By step 3.1 and [F7], ∑k∈Z∣h1/2f(hk)∣2=∥Φ(Gh)∥2=∥Gh∥2=∥f∥22. Since the left side is h∑k∣f(hk)∣2, dividing by h gives ∑k∣f(hk)∣2=h−1∥f∥L2(R)2, and in particular (h1/2f(hk))k∈Z∈ℓ2(Z).

Depends on

Used by

Dependency tree · two levels

108 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources