A real random variable is a measurable map from to with its Borel sigma-algebra. Equivalently, for every real . Its cumulative distribution function is
It is nondecreasing, right-continuous, and tends to zero and one at the two infinities.
Let be the distribution measure of . The measurable change-of-variables rule for expectations gives
For the second equality, let be uniform on and . The quantile function is measurable and satisfies
This equivalence uses monotonicity and right-continuity of . Consequently : has the same distribution as . In particular , so the signed integral is legitimate. Hence the quantile expectation formula is
No continuity or strict increase of the distribution function is required.
The variables are independent and identically distributed if they all have one common probability distribution and every finite selection satisfies
for distinct indices and arbitrary Borel sets. The condition concerns joint distributions, not merely pairwise correlations.
The strong law of large numbers states that if are independent and identically distributed real random variables with , then
The first absolute moment condition is part of the standard statement.
The zero means and orthogonality give the exact second moment
Thus in . Chebyshev's inequality gives the requested weak law of large numbers:
Independence is unnecessary; the stated second-moment orthogonality is sufficient.
For an explicit almost surely convergent subsequence take . For each positive integer ,
The First Borel-Cantelli lemma makes only finitely many such exceedances occur. Intersecting the resulting probability-one events over gives almost surely.

Articles by others on the same topic (0)

There are currently no matching articles.