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Strong-mixing CLTs under bounded, moment, and logarithmic-moment conditions

Statement

Assume AC. Let (Yk)k≥0 be a centered strictly stationary real sequence with E[Y02]<∞, and define Sn=∑k=1nYk. Each of the following is sufficient:

  1. There is B<∞ with ∣Y0∣≤B almost surely and ∑n≥1αY(n)<∞.
  2. For some δ>0, E∣Y0∣2+δ<∞ and ∑n≥1αY(n)δ/(2+δ)<∞.
  3. For some a∈(0,1), αY(n)=O(an) and E[Y02log⁡+∣Y0∣]<∞, where log⁡+u=max⁡(0,log⁡u) for u>0 and 0log⁡+0:=0.

In each case the covariance series σY2:=E[Y02]+2∑k=1∞Cov⁡(Y0,Yk) converges absolutely and is nonnegative, and n−1/2Sn⇒N(0,σY2). This includes the degenerate law N(0,0) when σY2=0, as in Zero covariance long-run variance gives a degenerate CLT under absolute summability. The coefficient αY and strict stationarity have the meanings in Strong, uniform, and maximal-correlation mixing coefficients.

Facts & Assumptions

Given: AC, the centered strictly stationary square-integrable real sequence, and one of the three sufficient regimes.

[A1]

AC is assumed for the bounded CLT, normal-law characteristic function and characteristic-function convergence criterion. (The Axiom of Choice)

[F1]

A centered bounded stationary real sequence with summable strong-mixing coefficients has an absolutely summable covariance series and a CLT with its nonnegative covariance-sum variance, including variance zero. (Bounded stationary CLT under summable strong mixing)

[F2]

Absolute tail quantiles have the original absolute-value law under uniform Lebesgue measure; square-integrable variables from fields with event coefficient a satisfy ∣Cov⁡(U,V)∣≤4∫0aQUQV. (Strong-mixing covariance bound in terms of tail quantiles)

[F3]

A measurable scalar observation preserves strict stationarity and does not increase the strong-mixing coefficients. (A measurable observation does not increase stationary mixing coefficients)

[F4]

Dominated convergence applies on arbitrary measure spaces and therefore also to absolutely dominated covariance series. (Dominated convergence)

[F5]

Tonelli interchanges nonnegative product integrals, including integration against counting measure. (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product)

[F6]

Holder's integral inequality holds for conjugate finite exponents on every measure space. (Holder's inequality for integrals, including the endpoint cases)

[F7]

Cauchy–Schwarz bounds absolute product expectations of square-integrable real variables. (Cauchy-Schwarz for random variables)

[F8]

Under AC the characteristic function of N(0,s2) is e−s2t2/2, including s=0. (Characteristic function of a normal law)

[F9]

Under AC, weak convergence to a specified probability law is equivalent to pointwise convergence of characteristic functions to that of the law. (Characteristic function criterion for weak convergence)

[F10]

Zero covariance-sum variance and absolute covariance summability give convergence of normalized sums in L2 and in distribution to N(0,0). (Zero covariance long-run variance gives a degenerate CLT under absolute summability)

[F11]

Variance and covariance are centered product expectations. (Moments, variance, and covariance on a probability space)

[F12]

The coefficient αY(n) is the event supremum for the past and the future separated by n. (Strong, uniform, and maximal-correlation mixing coefficients)

Proof

1.1A1F1F2F5givenalgebra

Write Q=QY0 for the absolute tail quantile in [F2], and put w(u)=1+∑r≥11{u<αY(r)} and J=∫01w(u)Q(u)2 du. We first show in every stated regime that J<∞ and ∑rαY(r)<∞. In regime 1, Q≤B and [F5] give J≤B2(1+∑rαY(r))<∞. This regime also already follows directly from [F1].

2.1F2F5F6F12step 1.1givenalgebra

In regime 2 put p=2+δ and θ=1−2/p=δ/(2+δ)∈(0,1). Holder's inequality [F6] with exponents p/2 and p/(p−2), followed by the quantile identity [F2], gives ∫0αY(r)Q(u)2 du≤αY(r)θ(∫01Q(u)p du)2/p=αY(r)θ(E∣Y0∣p)2/p. Tonelli [F5] and the assumed summability yield J<∞. Also 0≤αY(r)≤1 by its event definition, so αY(r)≤αY(r)θ, proving unweighted summability.

2.2F2step 1.1givenalgebra

In regime 3, choose constants C<∞ and a∈(0,1) so αY(r)≤Car outside a finite set of lags. Counting the positive integers satisfying u<Car shows w(u)≤C1+C2log⁡(1/u) for 0<u<1, with finite nonnegative constants C1,C2; also ∑rαY(r)<∞. The elementary inequality xv≤xlog⁡+x+ev for x,v≥0 follows for x>0 by maximizing xv−xlog⁡x+x as a function of x, whose maximum is ev; x=0 is immediate. Set x=Q(u)2 and v=12log⁡(1/u), then integrate and use [F2]: ∫01Q(u)2log⁡(1/u) du≤2∫01Q(u)2log⁡+(Q(u)2) du+2∫01u−1/2 du=4E[Y02log⁡+∣Y0∣]+4<∞. Together with the assumed second moment this proves J<∞. Thus the two properties announced in step 1.1 hold in all three regimes, without imposing a power moment in regime 3.

3.1F2F4F5F11F12step 1.1step 2.1step 2.2algebra

Let γr=Cov⁡(Y0,Yr). By [F2], [F12] and [F5], ∑r≥1∣γr∣≤4∑r≥1∫0αY(r)Q(u)2 du=4∫01(w(u)−1)Q(u)2 du<∞. Set DY=γ0+2∑r≥1∣γr∣. Expanding a finite centered sum over I⊆N0 and counting at most ∣I∣ pairs at each positive lag gives E(∑i∈IYi)2≤DY∣I∣. For consecutive sums the exact expression is Var⁡(Sn)/n=γ0+2∑r=1n−1(1−r/n)γr. The summable majorant and [F4] prove convergence to the stated σY2, which is nonnegative as a limit of nonnegative variances.

3.2A1F1F3step 1.1step 2.1step 2.2construct

For an integer M≥1 put cM(y)=max⁡(−M,min⁡(y,M)), Zk(M)=cM(Yk)−EcM(Y0), and HM(y)=y−cM(y). Then Rk(M)=Yk−Zk(M)=HM(Yk)−EHM(Y0). Both processes are strictly stationary by [F3], and Z(M) is centered and bounded by 2M. Its coefficients are bounded by αY, whose sum is finite by steps 1.1, 2.1, 2.2. Thus [F1] gives an absolutely convergent covariance series with nonnegative sum σM2, normalized variance convergence to σM2, and n−1/2∑k=1nZk(M)⇒N(0,σM2).

4.1F2F4F5F11F12step 1.1step 2.1step 2.2step 3.1step 3.2algebra

Put tM=P(∣Y0∣>M) and let QHM be the absolute quantile of HM(Y0). Since ∣HM(Y0)∣=(∣Y0∣−M)+≤∣Y0∣, monotonicity of tail probabilities gives QHM(u)≤Q(u), while QHM(u)=0 for u≥tM by its defining infimum. The centering in R(M) does not change any covariance, and Var⁡(HM(Y0))≤EHM(Y0)2. Applying [F2] to the raw, uncentered HM(Yk), followed by [F5], therefore gives DR(M):=E(R0(M))2+2∑r≥1∣Cov⁡(R0(M),Rr(M))∣≤8∫0tMw(u)Q(u)2 du=:eM2. Here the integrand is integrable by steps 1.1, 2.1, 2.2, and tM→0 because Y0 is finite almost surely; hence [F4] makes eM→0. The same finite covariance expansion as in step 3.1 now gives sup⁡n∥n−1/2∑k=1nRk(M)∥2≤eM. This bound uses the raw remainder quantile, without asserting that the centered remainder has that quantile.

5.1F7step 3.1step 3.2step 4.1algebra

The reverse triangle inequality for L2 norms gives ∣∥Sn/n∥2−∥n−1/2∑k=1nZk(M)∥2∣≤eM by step 4.1. This norm inequality follows by expanding a square and applying [F7] to its mixed term. Using the variance limits in steps 3.1 and 3.2 yields ∣σY−σM∣≤eM, where the square roots are nonnegative. Therefore σM→σY.

6.1A1F7F8F9F10step 3.1step 3.2step 4.1step 5.1∎

For fixed real t, ∣eix−eiy∣≤∣x−y∣, obtained by integrating the unit-modulus derivative along the real interval, and [F7] give ∣EeitSn/n−Eeit∑k=1nZk(M)/n∣≤∣t∣eM. By the CLT in step 3.2 and [F9], the second characteristic function tends to e−t2σM2/2, identified by [F8]. Consequently lim sup⁡n→∞∣EeitSn/n−e−t2σY2/2∣≤∣t∣eM+∣e−t2σM2/2−e−t2σY2/2∣. Let M→∞ and apply step 5.1. Under [A1], [F8]–[F9] prove Sn/n⇒N(0,σY2). The case σY2=0 is also independently supplied by [F10] using absolute covariance summability from step 3.1. All three regimes and the degenerate case follow.

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