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Fejer convolution formula for the lattice periodogram

Statement

Let d≥1 and let (Yj)j∈Zd be real square-integrable random variables with constant mean μ and lag-dependent covariance c(h):=Cov⁡(Yj+h,Yj), independent of j. Assume the Axiom of Choice and Dependent Choice. Then there is a unique finite positive Radon measure F on the angular torus Td such that c(h)=∫Tdeih⋅θ F(dθ),h∈Zd. For the periodogram In of Regular-grid spatial periodogram and smoothed estimator, define the product Fejer kernel Φn(x):=1(2π)dnd∣∑j∈{0,…,n−1}de−ij⋅x∣2=∏r=1d12πn∣∑a=0n−1e−iaxr∣2. Then, for every n≥1 and λ∈Td, E[In(λ)]=∫TdΦn(λ−θ) F(dθ). The kernel is nonnegative and has integral one with respect to product angular Lebesgue measure. The spectral measure and density here belong to the lattice-indexed observations on the dual torus.

Facts & Assumptions

Given: The lattice field, constant mean, covariance convention, and periodogram definition in the Statement; assume AC and DC.

[A1]

The Axiom of Choice: the Axiom of Choice is assumed.

[F1]

Positive definite functions on an abelian group: a function c:G→C is positive definite when every finite quadratic form ∑r,saras‾ c(xr−xs) is nonnegative.

[F2]

Bochner's theorem for LCA groups: under AC and DC, every continuous positive-definite function on an LCA group has a unique finite positive Radon representing measure on its Pontryagin dual.

[F3]

The Pontryagin dual of the integer lattice is the torus: Zd^ is identified with the product torus by χθ(j)=eij⋅θ.

[F4]

Transport of a lattice spectral measure to torus coordinates: a finite positive Radon measure on Zd^ transports to a finite positive Radon measure on Td while preserving integrals after composition.

[F5]

Regular-grid spatial periodogram and smoothed estimator: for Λn={0,…,n−1}d and Nn=nd, In(λ)=1(2π)dNn∣∑j∈Λn(Yj−μ)e−ij⋅λ∣2.

[F6]

Moments, variance, and covariance on a probability space: covariance is the expected centered product of square-integrable real random variables.

[F7]

Linearity, monotonicity, and the modulus bound for expectation and Cauchy-Schwarz for random variables: expectation is linear on finite integrable sums, and products of square-integrable variables are integrable.

[F8]

The product measure of two sigma-finite measure spaces and Fubini's theorem for L^1 functions on a sigma-finite product: the product angular Lebesgue measure exists and integrals can be evaluated by sections.

[F9]

The integer lattice is a discrete locally compact abelian group: Zd with the discrete topology is Hausdorff, abelian and locally compact, and every function on it is continuous.

[F10]

Integer exponentials are orthogonal for angular Lebesgue measure: under Countable Choice, for every integer k, ∫−ππeikx dx is 2π when k=0 and zero otherwise.

[F11]

AC implies DC implies countable choice: AC implies Countable Choice (through DC).

[F12]

The Axiom of Countable Choice (ACω): Countable Choice selects one element from each set in a countable family of nonempty sets.

Proof

Proof technique: prove the covariance sequence is positive definite, apply Bochner on the discrete lattice, then expand the finite Fourier square.

1.1F1F6F7givenalgebra

For any finite lattice points k1,…,km∈Zd and complex coefficients a1,…,am, the finite sum ∑rar(Ykr−μ) is square-integrable. Expanding its squared modulus, using [F6] and stationarity, gives ∑r,saras‾c(kr−ks)=E∣∑rar(Ykr−μ)∣2≥0. Thus c is positive definite by [F1].

1.2A1A2F2F9given

By [F9], Zd is a locally compact Hausdorff abelian group and every function on it is continuous, so c is continuous. By Bochner's theorem [F2], using AC [A1] and DC [A2], there is a unique finite positive Radon measure F0 on Zd^ such that c(h)=∫Zd^χ(h) F0(dχ).

1.3F5F6F7givenalgebra

Expand the finite squared modulus in [F5]. Every product is integrable by [F7], and stationarity gives E[In(λ)]=1(2π)dnd∑j,k∈Λnc(j−k)e−i(j−k)⋅λ.

2.1F3F4step 1.2

By [F3] and [F4], transport F0 to the unique finite positive Radon measure F on Td. Applying the integral-transport identity [F4] to χ↦χ(h) gives c(h)=∫Tdeih⋅θ F(dθ).

3.1F5step 2.1step 1.3F7algebra

Substitute the spectral representation from step 2.1 into each summand of step 1.3. Linearity permits moving the finite sum through the integral, and ∑j,k∈Λne−i(j−k)⋅(λ−θ)=∣∑j∈Λne−ij⋅(λ−θ)∣2. After dividing by (2π)dnd this is precisely E[In(λ)]=∫TdΦn(λ−θ) F(dθ).

4.1A1F8F10F11F12algebra∎

The displayed kernel factors into nonnegative one-dimensional kernels. For each coordinate, expanding the finite square and applying angular orthogonality [F10] to each integer exponent a−b gives ∫−ππ12πn∣∑a=0n−1e−iax∣2dx=1. The Countable Choice hypothesis of [F10] follows from AC by [F11] and [A1]. Fubini [F8] for the finite product then gives ∫TdΦn(x) dx=1, and nonnegativity follows from the squared modulus.

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