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A geometrically summable Bernoulli shift

Statement

Let (ϵt)t∈Z be iid Rademacher variables, put e(u)=1 in H=L2([0,1],dt;R), and define Xt=(∑k=0∞2−kϵt−k)e. The series converges absolutely for every sign sequence. Its physical dependence coefficients are δm2=83 4−m, so they are summable. Its long-run covariance is 4(e⊗e), and under AC the Hilbert-valued CLT gives a centered Gaussian limit with that covariance.

Facts & Assumptions

Given: AC and countably many iid Rademacher innovations.

[A1]

AC supplies Countable Choice and the countable independent family used here (The Axiom of Choice, Countably many independent copies of a prescribed law exist).

[F1]

For fixed m, the replacement keeps coefficients k<m and uses independent copies for all k≥m; δm is the resulting L2(H) error (L2-m-approximable causal Bernoulli shifts).

[F2]

The stated two-point Rademacher law gives mean zero and variance one; independence means independence of the generated sigma-algebras, and expectations of independent integrable products factor (Expectation of a nonnegative or integrable random variable, Independent random elements, Expectations factor over finite products of independent random variables). Dominated convergence passes expectations through uniformly bounded partial sums (Dominated convergence).

[F3]

Under AC, a centered L2-approximable causal shift has the Hilbert valued CLT with its long-run covariance operator (Hilbert-valued CLT for L2-m-approximable Bernoulli shifts).

Proof

Given: The innovations and process in the Statement.

1.1A1F1F2constructalgebra

For every input sequence with ∣ϵt∣=1, ∑k≥0∣2−kϵt−k∣≤2, so the series converges absolutely and uniformly over the product space. Its partial sums are product-measurable and bounded by 2, so their pointwise limit is a Borel causal map. Finite partial-sum variances are ∑k≤N4−k by [F2]; the uniform bound and dominated convergence give centering and E∥X0∥H2=∑k≥04−k=4/3<∞. For the replacement, the first m terms cancel; finite tails are independent centered differences with variance 2∑k=mN4−k and are bounded in absolute value by 2∑k=m∞2−k. Dominated convergence [F2] passes these variances to the infinite tail, giving δm2=2∑k=m∞4−k=83 4−m. Thus ∑m≥1δm=8/3∑m≥12−m<∞.

2.1F2step 1.1algebra

For j≥0, truncate both linear sums at index N. Their product is bounded by 4 and converges pointwise to X0Xj, so dominated convergence [F2] passes expectations to the limit. The finite sums share exactly innovations with indices −k=j−(k+j); their coefficient products are 2−k2−(k+j), while all other products have zero expectation by [F2]. The finite shared-coefficient sums tend to ∑k≥02−k2−(k+j), giving γj=E⟨X0,Xj⟩H=43 2−j. Symmetry gives γ−j=γj. Therefore the scalar long-run variance is γ0+2∑j≥1γj=43+83∑j≥12−j=4, and the operator is 4(e⊗e).

3.1F3step 1.1step 2.1∎

Step 1.1 gives centering, a finite second moment and summable physical-dependence errors; step 2.1 gives the long-run covariance. Applying [F3] yields convergence of the normalized H-valued sums to a centered Gaussian with covariance 4(e⊗e).

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