How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Green–Kubo covariance limit under absolute integrability
Statement
Let be a probability space and let be jointly measurable for the completed product of Lebesgue measure and . Assume for every , , and second-order stationarity in the explicit sense that each covariance below is finite and is independent of for every and every . For , the Lebesgue integral exists almost surely and in . Define the centered hypothesis makes these means zero. Then If each is absolutely integrable on , then and 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.
is assumed for the completed-product Tonelli–Fubini supplier (The Axiom of Countable Choice ()).
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 hypothesis.
Dominated convergence: almost-everywhere convergence under one common integrable majorant allows passage to the limit in the integral.
Integrable real and complex functions, and their integrals: and denote absolute integrability of the corresponding powers with respect to the indicated measure.
Cauchy-Schwarz inequality for : the integral Cauchy–Schwarz inequality applies to square-integrable functions.
Proof
Given: [A1] and the process hypotheses in the statement.
By second-order stationarity, for every . Tonelli applied to the nonnegative jointly measurable function therefore gives . Consequently the path integral of is finite almost surely; [F4] on then makes pathwise integrable. Moreover, , so .
The bound in step 1.1 and Cauchy–Schwarz in probability give . Fubini and therefore give . For each , [F4] and stationarity give on the finite square . Fubini therefore permits expansion of as the double integral of . Splitting the square into and , then writing , gives the two terms and . Since the means are zero, this is the stated covariance formula.
Divide the covariance formula by and extend the integrand by zero for . Its entry is . As it converges pointwise to and is bounded by the integrable function . By [F2], each matrix entry converges to the stated integral.
For every , because it is a scaled variance. Entrywise convergence from step 3.1 gives . Thus is positive semidefinite. For a scalar velocity observable in units m/s, has units m/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.