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Green–Kubo covariance limit under absolute integrability

Statement

Let (Ξ,F,P) be a probability space and let V:R×Ξ→Rd be jointly measurable for the completed product of Lebesgue measure and P. Assume E[V(t)]=0 for every t, E∣V(0)∣2<∞, and second-order stationarity in the explicit sense that each covariance below is finite and Cij(s):=E[Vi(u)Vj(u+s)] is independent of u∈R for every s∈R and every 1≤i,j≤d. For T>0, the Lebesgue integral X(T)=∫0TV(s) ds exists almost surely and in L2. Define Cov⁡(X(T))ij=E[(Xi(T)−EXi(T))(Xj(T)−EXj(T))]; the centered hypothesis makes these means zero. Then Cov⁡(Xi(T),Xj(T))=∫0T(T−s)(Cij(s)+Cji(s)) ds. If each Cij is absolutely integrable on [0,∞), then Cov⁡(X(T))2T⟶D,Dij=12∫0∞(Cij(s)+Cji(s)) ds, and D is positive semidefinite. This is a variance-growth conclusion; it does not assert a central limit theorem or identify a transport coefficient.

Facts & Assumptions

Given: A probability space, a jointly measurable centered vector process with stationary second moments and finite second moment at one time, plus absolute integrability of every nonnegative-lag covariance entry for the limit clause.

[A1]

ACω is assumed for the completed-product Tonelli–Fubini supplier (The Axiom of Countable Choice (ACω)).

[F1]

Tonelli and Fubini for the completed product, with only almost-everywhere section measurability: on a completed product of sigma-finite spaces, nonnegative integrals and integrable functions may be integrated by sections under its stated ACω hypothesis.

[F2]

Dominated convergence: almost-everywhere convergence under one common integrable majorant allows passage to the limit in the integral.

[F3]

Integrable real and complex functions, and their integrals: L1 and L2 denote absolute integrability of the corresponding powers with respect to the indicated measure.

[F4]

Cauchy-Schwarz inequality for L2: the integral Cauchy–Schwarz inequality applies to square-integrable functions.

Proof

Given: [A1] and the process hypotheses in the statement.

1.1A1F1F3F4givenalgebra

By second-order stationarity, E∣V(t)∣2=∑iCii(0)=E∣V(0)∣2 for every t. Tonelli applied to the nonnegative jointly measurable function ∣V∣2 therefore gives E∫0T∣V(s)∣2 ds=TE∣V(0)∣2<∞. Consequently the path integral of ∣V∣2 is finite almost surely; [F4] on [0,T] then makes V pathwise integrable. Moreover, ∣X(T)∣2≤T∫0T∣V(s)∣2ds, so X(T)∈L2.

2.1F1F4step 1.1givenalgebra

The bound in step 1.1 and Cauchy–Schwarz in probability give E∫0T∣V(s)∣ ds≤T(E∣V(0)∣2)1/2<∞. Fubini and E[V(s)]=0 therefore give E[X(T)]=0. For each i,j, [F4] and stationarity give E∣Vi(u)Vj(v)∣≤E∣V(0)∣2 on the finite square [0,T]2. Fubini therefore permits expansion of E[Xi(T)Xj(T)] as the double integral of E[Vi(u)Vj(v)]. Splitting the square into u≤v and v≤u, then writing s=∣v−u∣, gives the two terms ∫0T(T−s)Cij(s)ds and ∫0T(T−s)Cji(s)ds. Since the means are zero, this is the stated covariance formula.

3.1A1F2step 2.1

Divide the covariance formula by 2T and extend the integrand by zero for s>T. Its (i,j) entry is 121[0,T](s)(1−s/T)(Cij(s)+Cji(s)). As T→∞ it converges pointwise to 12(Cij(s)+Cji(s)) and is bounded by the integrable function 12(∣Cij(s)∣+∣Cji(s)∣). By [F2], each matrix entry converges to the stated integral.

4.1step 3.1algebra∎

For every a∈Rd, a⊤Cov⁡(X(T))a/(2T)≥0 because it is a scaled variance. Entrywise convergence from step 3.1 gives a⊤Da=lim⁡T→∞a⊤Cov⁡(X(T))a/(2T)≥0. Thus D is positive semidefinite. For a scalar velocity observable in units m/s, D has units m2/s.

Remarks

The MIT notes derive a self-diffusion formula from a physical long-time mean-square-displacement assumption. The theorem here proves only the stated covariance limit under second-order stationarity and absolute integrability; it supplies neither that physical identification nor a Gaussian limit.

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