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The Dirac comb of a full-rank lattice transforms to the dual comb

Statement

Assume Countable Choice (The Axiom of Countable Choice (ACω)). Let Λ be a full-rank lattice with covolume c and dual Λ∗. The Λ-Dirac comb comb⁡Λ:=∑λ∈Λδλ, defined by ⟨comb⁡Λ,φ⟩=∑λφ(λ), is a tempered distribution, and Fcomb⁡Λ=c−1comb⁡Λ∗in S′(Rn), that is, ⟨Fcomb⁡Λ,φ⟩=c−1∑λ∗∈Λ∗φ(λ∗) for every φ∈S(Rn). For Λ=Zn (c=1, Λ∗=Zn) this is Fourier-invariance of the unit comb, the published Dirac comb is fourier invariant; the scaled case here (Λ=hZn, c=hn) is what the sampling lemma below consumes.

Facts & Assumptions

Given: Countable Choice, the full-rank lattice Λ=AZn with covolume c and dual Λ∗=A−TZn (Full-rank lattices, covolume, and the dual lattice), the Dirac distributions δλ (Dirac delta and its derivatives), and the unit comb conventions of Dirac comb.

[F1]

For every integer L≥0 and every x∈Rn, ∣φ(x)∣≤An,L(1+∣x∣)−Lmax⁡∣α∣≤Lpα,0(φ). Indeed 1+∣x∣≤1+∑j∣xj∣, whose Lth power is a finite sum of monomials ∣xα∣ with ∣α∣≤L and positive coefficients by The multinomial coefficient equals n!/∏i<mki!, and (x0+⋯+xm−1)n=∑ι ⁣(nk)∏i<mxiki in R; multiplying by ∣φ(x)∣ bounds each monomial by its seminorm (Schwartz space and its seminorms). At integer points this is the unit-comb estimate of Dirac comb.

[F2]

Transporting shells by λ=Ak: ∣λ∣≤r implies ∣k∣≤Kr for a constant K, and conversely m≤∣λ∣<m+1 implies m/K′≤∣k∣<K′(m+1) for constants, so the shell has at most C(1+m)n lattice points; likewise for Λ∗=A−TZn (Every Euclidean linear map has a unique matrix and satisfies ∥Lh∥2≤K∥h∥2 for some K≥0, Full-rank lattices, covolume, and the dual lattice).

[F3]

∑m≥1mn−L<∞ for real L>n+1; a finite-seminorm bound characterises tempered distributions (The p-series for a real exponent p converges exactly when p is greater than one, Finite seminorm bound characterizes tempered distributions).

[F4]

The Fourier transform of a tempered distribution is defined by ⟨Fu,φ⟩=⟨u,Fφ⟩ (Fourier transform of a tempered distribution), and on Schwartz functions F2=R with Rφ(x)=φ(−x) (Fourier transform is a topological automorphism of Schwartz space).

[F5]

Poisson summation for a full-rank lattice: for ψ∈S(Rn), ∑λ∈Λψ(λ)=c−1∑λ∗∈Λ∗ψ^(λ∗) (Poisson summation for a full-rank lattice).

Proof

technique · direct
1.1F1F2F3givenalgebra

Fix an integer L>n+1. For φ∈S, the bound of [F1] and the shell count of [F2] give ∑λ∈Λ∣φ(λ)∣≤An,L∑m≥0C(1+m)n(1+m)−Lmax⁡∣α∣≤Lpα,0(φ), which is finite by [F3]; hence the series defining comb⁡Λ converges absolutely and satisfies a single finite-seminorm estimate, so comb⁡Λ is a tempered distribution by [F3]. On a compactly supported test only finitely many δλ remain, matching the locally finite sum of Dirac delta and its derivatives, so the definition is the intended one.

2.1step 1.1F4F5givenalgebra

For φ∈S, the definition of the distributional transform [F4] and the definition of the comb give ⟨Fcomb⁡Λ,φ⟩=⟨comb⁡Λ,Fφ⟩=∑λ∈Λφ^(λ). Applying the lattice Poisson formula [F5] to the Schwartz function ψ:=φ^, and using F2=R on Schwartz functions [F4], ∑λφ^(λ)=c−1∑λ∗φ^^(λ∗)=c−1∑λ∗φ(−λ∗). The map λ∗↦−λ∗ is a bijection of the group Λ∗, so the last sum equals c−1∑λ∗φ(λ∗)=⟨c−1comb⁡Λ∗,φ⟩.

3.1step 2.1F5given∎

Equality of the two tempered distributions on every Schwartz test proves Fcomb⁡Λ=c−1comb⁡Λ∗; at Λ=Zn, where c=1 and Λ∗=Zn, this specialises to the published unit-comb theorem Dirac comb is fourier invariant, which is hereby a cross-check rather than a supplier. Countable Choice is inherited from the Poisson theorem and the distributional Fourier interface.

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