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Variance adds for every finite pairwise-independent family
Statement
If is a finite pairwise-independent family of square-integrable real random variables on a common probability space, then Pairwise independence, rather than mutual independence, is sufficient. In particular, the original finite-probability-space case is included, with pairwise atom independence as in the finite-valued convention. The empty sum has variance zero.
Facts & Assumptions
Given: A finite pairwise-independent family of square-integrable real random variables on one probability space.
Expectations of products of independent integrable real random variables factor; the finite-valued atom-independence convention is included. (Expectation factors over a finite product of mutually independent random variables)
For square-integrable real random variables, covariance equals , is symmetric and bilinear on finite linear combinations, and variance equals the self-covariance. These identities agree with the original finite-space definitions. (Variance and covariance identities for random variables)
Proof
Each is integrable because and the measure has total mass one. For distinct , pairwise independence and [L1] give , so [L2] gives .
The finite sum is square-integrable: repeated use of gives an integrable bound for . By [L2], where step 1.1 removes all off-diagonal terms. The empty sum is the constant zero, and the singleton case is the identity.
Depends on
Used by
- Chebyshev bounds the majority error of repeated Bernoulli trials Lemma
- Finite two-stage sampling variance identities Lemma
- Coefficient and factorial-effect variances under equal replication Theorem
- Expected mean squares in the balanced one-way normal random-effects model Theorem
- Ordinary importance sampling has finite variance and a CLT under a weighted second moment Theorem
- Unbiasedness and exact variance of the IID Monte Carlo mean Theorem
Dependency tree · two levels
11 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- C. M. Grinstead and J. L. Snell, Introduction to Probability, 2nd ed., Theorem 6.4 (standard reference, not scraped)
- J. Matousek and J. Vondrak, The Probabilistic Method, Section 6.1 (standard reference, not scraped)