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Pairwise-independent Borel-Cantelli frequency law

Statement

Let (An)n≥1 be pairwise independent events with ∑n=1∞P(An)=+∞. For n≥1, put Sn:=∑k=1n1Ak,an:=∑k=1nP(Ak). Then an>0 for all sufficiently large n, and for those n Then Snan⟶1almost surely.

Facts & Assumptions

Given: Pairwise independent events (An)n≥1 with ∑n=1∞P(An)=+∞, and the sums Sn,an of the Statement.

[L1]

Pairwise independence means P(Ai∩Aj)=P(Ai)P(Aj)(i≠j). (Pairwise independence)

[L2]

An indicator of a measurable event is a real random variable, and its expectation is the probability of the event. (An indicator function is measurable exactly when its set is measurable, The expectation of an indicator is the probability of the event)

[L3]

Finite sums, products, and absolute values of measurable real-valued functions are measurable. (Arithmetic and lattice operations preserve measurability whenever they are defined)

[L4]

Expectation is linear on integrable random variables, and Var⁡(X)=E[X2]−E[X]2 for square-integrable real random variables. (Linearity, monotonicity, and the modulus bound for expectation, Variance and covariance identities for random variables)

[L5]

Chebyshev's inequality bounds the probability of a centered deviation by variance divided by the square threshold. (Chebyshev's inequality for random variables)

[L6]

If a sum of event probabilities is finite, then the corresponding limsup event has probability zero. (First Borel-Cantelli lemma for events)

Proof

technique · direct
1.1givenL2L4

For each k, the indicator 1Ak is a real random variable by [L2]. Repeated use of [L4] and [L2] gives E[Sn]=∑k=1nE[1Ak]=∑k=1nP(Ak)=an. The divergence hypothesis makes an→+∞. In particular, there is N≥1 with an>0 for every n≥N.

2.1step 1.1L1L2algebra

For i≠j, step 1.1 and [L1] give E[1Ai1Aj]=E[1Ai∩Aj]=P(Ai∩Aj)=P(Ai)P(Aj)=E[1Ai] E[1Aj]. Also 1Ak2=1Ak for every k.

3.1step 1.1step 2.1L3L4algebra

By [L3], the partial sum Sn and its square Sn2 are measurable. Expanding Sn2 and using step 2.1 together with linearity from [L4] yields E[Sn2]=∑k=1nP(Ak)+2∑1≤i<j≤nP(Ai)P(Aj)=an2+∑k=1n(P(Ak)−P(Ak)2)≤an2+an. So Sn is square-integrable, and [L4] gives Var⁡(Sn)=E[Sn2]−E[Sn]2≤an.

4.1step 1.1step 3.1L5algebra

Fix ε>0 and n≥N. Applying [L5] to Sn gives P(∣Snan−1∣≥ε)=P(∣Sn−an∣≥εan)≤Var⁡(Sn)ε2an2≤1ε2an. Hence Sn/an→1 in probability along the defined tail n≥N.

5.1step 1.1step 4.1algebra

For each integer m≥1, let nm be the least index with anm≥a1+m2; it exists by step 1.1. Since anm−1<a1+m2≤anm and anm−anm−1=P(Anm)≤1, one has a1+m2≤anm<a1+m2+1. Therefore step 4.1 yields P(∣Snmanm−1∣≥ε)≤1ε2(a1+m2), and the sum over m is finite.

6.1step 5.1L6

For each integer r≥1, step 5.1 with ε=1/r gives ∑m=1∞P(∣Snmanm−1∣≥1r)<+∞. Applying [L6] to these deviation events shows that, for each r, only finitely many of them occur almost surely.

7.1step 6.1algebra

Intersect the full-probability events from step 6.1 over all r∈N>0. On that still full-probability event, for every r there is Mr(ω) such that ∣Snm(ω)anm−1∣<1r(m≥Mr(ω)). Hence Snm/anm→1 almost surely.

8.1step 5.1step 7.1algebra

Fix ω in the full-probability event from step 7.1. If nm≤n<nm+1, then Snm(ω)≤Sn(ω)≤Snm+1(ω) and anm≤an<anm+1, so Snm(ω)anm+1≤Sn(ω)an≤Snm+1(ω)anm. Since anm/anm+1→1 and anm+1/anm→1 by the bounds in step 5.1, step 7.1 squeezes Sn(ω)/an to 1. Therefore Sn/an→1 almost surely for all sufficiently large n, equivalently for all n with an>0.

9.1step 8.1∎

Step 8.1 is exactly the asserted frequency law.

Depends on

Used by

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Sources