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Weak Laws and Series of Independent Random Variables — Examples

1 · Prerequisites

2 · Summary

These examples distinguish IID hypotheses, variance control, tail control, and absolute convergence. Bernoulli sample means illustrate the weak laws; fair-sign series show the sharp square-summability threshold. Three constructions isolate the three-series conditions, while rare large jumps separate almost-sure convergence from summability of untruncated variances. Cauchy and logarithmic tails mark the boundary for deterministic weak-law centering.

Sequence-existence constructions retain the countable-choice and dependent-choice hypotheses of the countable product results.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: AI-adaptedVerification: AI-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07Open item page →

Bernoulli sample frequencies

Example

Assume countable choice and dependent choice. For IID Bernoulli(p) variables (Xk)k≥1, where 0≤p≤1, let Sn=∑k=1nXk. Then Sn/n→p in probability and P(∣Sn/n−p∣≥ε)≤p(1−p)nε2(ε>0). The endpoint laws p=0,1 are included.

Facts & Assumptions

[F1]

IID finite-variance weak law: Let (Xk)k≥1 be IID square-integrable real random variables, with μ=EX1 and σ2=Var⁡(X1). For Sn=∑k=1nXk, E∣Sn/n−μ∣2=σ2/n, and Sn/n→μ in L2 and in probability. Also P(∣Sn/n−μ∣≥ε)≤σ2/(nε2) for ε>0.

[F2]

Bernoulli random variables and binomial random variables as sums of independent Bernoulli trials: For p∈[0,1], a Bernoulli(p) random variable takes the value 1 with probability p and 0 with probability 1−p. For n∈N, a binomial(n,p) random variable is a sum X=∑i<nXi of n mutually independent Bernoulli(p) variables. When n=0, this is the constant zero random variable.

[F3]

A Bernoulli(p) variable has mean p and variance p(1−p); a binomial(n,p) variable has mean np and variance np(1−p): If X is Bernoulli(p), then E[X]=p and Var⁡(X)=p(1−p). If S is binomial(n,p), then E[S]=np,Var⁡(S)=np(1−p). These formulas include p=0, p=1, and n=0.

[F4]

Countably many independent copies of a prescribed law exist: Assume countable choice and dependent choice. Every probability measure ν on (S,Σ) is the common law of a countable independent family of S-valued random elements.

Verification

Given: The construction and assumptions above.

1.1F2F4F3given

The Bernoulli law puts masses p and 1−p at 1 and 0. Under countable choice and dependent choice, the countable-copy result constructs a common-space IID sequence with this law. Its mean is p and variance p(1−p), including both endpoints.

2.1F1step 1.1algebra∎

The finite-variance IID weak law and its probability bound apply with μ=p and σ2=p(1−p), giving the displayed estimate and convergence. If p=0 or p=1, all the variables equal p on the intersection of their countably many probability-one events, so every sample mean equals p there and the error probability is zero, even at n=1.

ExampleConstruction: AI-generatedVerification: AI-generatedverified 2026-09-23 (gpt-6-sol)Open item page →

A nonidentical Bernoulli weak law

Example

Assume countable choice and dependent choice. Let independent Xk be Bernoulli(pk) with pk=1/4 for odd k and pk=3/4 for even k. Then for Sn=∑k=1nXk, E∣Sn−ESnn∣2=316n,Sn/n⟶1/2in probability. Thus a common distribution is not required.

Facts & Assumptions

[F1]

Chebyshev weak law for uncorrelated arrays: For each n≥1, let Xn,1,…,Xn,rn be square-integrable real random variables on one probability space, pairwise uncorrelated within the row, where rn≥0 is finite. Set Sn=∑k=1rnXn,k and let bn>0 be deterministic. If vn:=bn−2∑k=1rnVar⁡(Xn,k)⟶0, then (Sn−ESn)/bn→0 in L2 and in probability. More precisely, its second moment is vn, and its probability of absolute value at least ε>0 is at most vn/ε2. No independence between rows is required.

[F2]

Coordinate random elements of a countable product are independent: Under the measure of thm-countable-product-of-probability-spaces, the coordinate maps Xn(x)=xn have laws μn and are independent.

[F3]

Assuming countable and dependent choice, countable products of arbitrary probability spaces: Assume countable choice and dependent choice. For probability spaces (En,En,μn)n∈N there is a unique probability measure μ on CN such that, for every finite F, its F-coordinate marginal is ⨂n∈Fμn.

[F4]

A Bernoulli(p) variable has mean p and variance p(1−p); a binomial(n,p) variable has mean np and variance np(1−p): If X is Bernoulli(p), then E[X]=p and Var⁡(X)=p(1−p). If S is binomial(n,p), then E[S]=np,Var⁡(S)=np(1−p). These formulas include p=0, p=1, and n=0.

[F5]

For n≥1, if X0,…,Xn−1 are independent real random variables and gi:R→R are Borel measurable with each gi(Xi) integrable, then ∏i<ngi(Xi) is integrable and E[∏i<ngi(Xi)]=∏i<nE[gi(Xi)] in R (Expectations factor over finite products of independent random variables).

Verification

Given: The construction and assumptions above.

1.1F3F2F4givenF5

Under countable choice and dependent choice, take the countable product of the two-point Bernoulli probability spaces with the prescribed pk (shift the product index by one). Its coordinates are independent with the required laws. Each has mean pk and variance 3/16. Independence gives zero mixed centered moments, hence zero off-diagonal covariances.

2.1F1step 1.1algebra∎

The row weak law with the first n entries and normalizer n gives centered second moment n(3/16)/n2=3/(16n) and convergence in probability to zero. Meanwhile ESn/n=1/2 for even n and 1/2−1/(4n) for odd n, including n=1. For any ε>0 the deterministic error is eventually below ε/2, so the probability of ∣Sn/n−1/2∣>ε is at most the probability that the centered average exceeds ε/2 in absolute value, which tends to zero.

ExampleConstruction: AI-adaptedVerification: AI-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07Open item page →

Rademacher-series threshold

Example

Assume countable choice and dependent choice, and let (ϵn)n≥1 be independent fair signs taking exactly the values −1 and 1. For real α, the series ∑n≥1ϵnn−α converges almost surely exactly when α>1/2; if α≤1/2 it diverges almost surely. Its absolute series converges exactly when α>1.

Facts & Assumptions

[F1]

Kolmogorov three-series theorem: Let (Xn)n≥1 be independent real random variables and fix A>0. Put Yn=Xn1{∣Xn∣≤A}. Then ∑nXn converges almost surely if and only if all three conditions hold: ∑nP(∣Xn∣>A)<∞,∑nEYn converges in R,∑nVar⁡(Yn)<∞. The conditions hold for some A>0 if and only if they hold for every A>0. No moment assumption is imposed on the untruncated variables.

[F2]

Almost-sure convergence of an independent series is a zero-one event: Let (Xn)n∈N be an independent sequence of real random variables. Then the event {∑n=0∞Xn converges} has probability 0 or 1.

[F3]

Countably many independent copies of a prescribed law exist: Assume countable choice and dependent choice. Every probability measure ν on (S,Σ) is the common law of a countable independent family of S-valued random elements.

[F4]

The p-series for a real exponent p converges exactly when p is greater than one: For every real p, ∑k≥11kp converges⟺p>1.

Verification

Given: The construction and assumptions above.

1.1F3givenalgebra

Under countable choice and dependent choice, construct IID copies of the probability law on the two-point space {−1,1}, each point having mass 1/2. For α>0, the summands have magnitude n−α≤1. At cutoff A=1, the tail probabilities and truncated means are zero, and the truncated variances are n−2α.

2.1F1F4F2step 1.1

The three-series theorem and the real p-series test therefore give almost-sure convergence for α>1/2 and rule out probability-one convergence for 0<α≤1/2. In the latter range the convergence event is a tail event of an independent sequence, so its zero-one law forces its probability to be zero. In particular the boundary α=1/2 has the divergent harmonic variance series.

3.1F4step 1.1algebra∎

If α≤0, the magnitudes n−α≥1 do not tend to zero at any point, so the partial sums cannot converge. Finally at every point the absolute series equals ∑nn−α, which converges exactly for α>1 by the p-series test. This also checks the absolute boundary α=1 and the term-test boundary α=0.

ExampleConstruction: AI-adaptedVerification: AI-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07Open item page →

Almost-sure conditional convergence

Example

Assume countable choice and dependent choice. On a probability space carrying independent fair signs ϵn∈{−1,1}, the random harmonic series ∑n≥1ϵn/n converges almost surely, but ∑n≥1∣ϵn/n∣ diverges at every sample point. By comparison the deterministic harmonic series diverges and its alternating version converges.

Facts & Assumptions

[F1]

Kolmogorov three-series theorem: Let (Xn)n≥1 be independent real random variables and fix A>0. Put Yn=Xn1{∣Xn∣≤A}. Then ∑nXn converges almost surely if and only if all three conditions hold: ∑nP(∣Xn∣>A)<∞,∑nEYn converges in R,∑nVar⁡(Yn)<∞. The conditions hold for some A>0 if and only if they hold for every A>0. No moment assumption is imposed on the untruncated variables.

[F2]

Countably many independent copies of a prescribed law exist: Assume countable choice and dependent choice. Every probability measure ν on (S,Σ) is the common law of a countable independent family of S-valued random elements.

[F3]

The p-series for a real exponent p converges exactly when p is greater than one: For every real p, ∑k≥11kp converges⟺p>1.

[F4]

The alternating series test: if (bk) is nonincreasing with bk→0 then ∑k(−1)kbk converges, the sum lies between any two consecutive partial sums, and the error after n terms is at most bn: Let (εk) be the alternating sequence of lem-alternating-sequence, that is the unique sequence of reals with ε0=1 and εk+1=−εk, which is what is usually written εk=(−1)k; let e and o be its even and odd index maps, so that εej=1, εoj=−1, and every natural number is ej for exactly one j or oj for exactly one j. Let (bk) be a sequence of reals that is nonincreasing (def-monotone-sequence) and converges to 0 (def-real-limit); then bk≥0 for every k. Write tn:=∑k<nεkbk for the partial sums (def-series). Then: 1. the series ∑εkbk converges; write L for its sum; 2. tej≤L≤toj for every j∈N, and for every n∈N the sum L lies between the two consecutive partial sums tn and tn+1; 3. ∣L−tn∣≤bn for every n∈N. Claim 3 is the error bound: the partial sum tn, which uses the n terms ε0b0,…,εn−1bn−1, differs from the sum by at most the first term omitted. Only claim 1 is a corollary of thm-dirichlet-test. Claims 2 and 3 are not: they come from the interlacing of the even-index and odd-index partial sums, and that argument is carried out below rather than smuggled into the Dirichlet estimate, which produces no bracketing at all.

Verification

Given: The construction and assumptions above.

1.1F2F3F1givenalgebra

Under countable choice and dependent choice, use the countable-copy theorem for the fair law on {−1,1}. At cutoff A=1, all summands Xn=ϵn/n are retained, including the first one. Their means are zero and their variances are 1/n2, whose sum is finite. Three-series therefore gives almost-sure convergence.

2.1F3F4step 1.1algebra∎

At every point ∣ϵn/n∣=1/n, and the harmonic p-series diverges. Thus on the probability-one convergence event the convergence is conditional. The same p-series test gives deterministic harmonic divergence. Apply the zero-based alternating-series test with bk=1/(k+1) to obtain convergence of ∑n≥1(−1)n−1/n; bk decreases to zero and is nonnegative.

ExampleConstruction: AI-generatedVerification: AI-generatedaudited 2026-09-07Open item page →

The three series impose separate conditions

Example

Assume countable choice and dependent choice. At cutoff A=1, each of the following independent-sequence constructions violates exactly one of the three-series conditions:

  1. For n≥2, let Xn=2 with probability 1/n and Xn=0 otherwise; set X1=0. Only the large-jump probability series diverges.
  2. Let Xn=1/n deterministically. Only the truncated mean series diverges.
  3. Let Xn=ϵn/n for independent fair signs. Only the truncated variance series diverges.

None of these series converges almost surely.

Facts & Assumptions

[F1]

Kolmogorov three-series theorem: Let (Xn)n≥1 be independent real random variables and fix A>0. Put Yn=Xn1{∣Xn∣≤A}. Then ∑nXn converges almost surely if and only if all three conditions hold: ∑nP(∣Xn∣>A)<∞,∑nEYn converges in R,∑nVar⁡(Yn)<∞. The conditions hold for some A>0 if and only if they hold for every A>0. No moment assumption is imposed on the untruncated variables.

[F2]

Second Borel-Cantelli lemma under pairwise independence: Let (An)n∈N be pairwise independent events with ∑n=0∞P(An)=+∞. Then P(An i.o.)=1.

[F3]

The p-series for a real exponent p converges exactly when p is greater than one: For every real p, ∑k≥11kp converges⟺p>1.

[F4]

Coordinate random elements of a countable product are independent: Under the measure of thm-countable-product-of-probability-spaces, the coordinate maps Xn(x)=xn have laws μn and are independent.

[F5]

Assuming countable and dependent choice, countable products of arbitrary probability spaces: Assume countable choice and dependent choice. For probability spaces (En,En,μn)n∈N there is a unique probability measure μ on CN such that, for every finite F, its F-coordinate marginal is ⨂n∈Fμn.

Verification

Given: The construction and assumptions above.

1.1F5F4F3F2given

Under countable choice and dependent choice, the countable product of the stated finite probability spaces constructs the first and third independent sequences; deterministic coordinates construct the second. In the first construction the zero truncations at 1 are all zero, so their mean and variance series vanish, but ∑n≥2P(∣Xn∣>1)=∑n≥21/n=∞. The second Borel–Cantelli lemma gives infinitely many terms equal to 2 almost surely; hence the terms fail to tend to zero.

1.2F3givenalgebra

For the second construction, every term is retained at A=1, its variance is zero, and there are no large jumps. Its truncated mean series is ∑n1/n=∞. Thus exactly the mean condition fails and its deterministic partial sums diverge.

2.1F3F1givenalgebra∎

For the third construction every term, including n=1, is retained, there are no large jumps, and the means vanish. Its variance series is ∑n1/n=∞. The three-series theorem rules out almost-sure convergence. Each construction therefore isolates exactly the claimed failed condition.

CounterexampleConstruction: AI-generatedVerification: AI-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07Open item page →

A macroscopic row term defeats averaging

Statement refuted

The assertion that independent centered rows automatically satisfy a weak law with normalization n is false. Assume countable choice and dependent choice. A witness is the row of length n defined by Xn,1=nϵn and Xn,k=0 for 2≤k≤n, where the ϵn are independent fair signs. With Sn=∑k=1nXn,k, Sn/n does not converge in probability to zero.

Facts & Assumptions

[F1]

Chebyshev weak law for uncorrelated arrays: For each n≥1, let Xn,1,…,Xn,rn be square-integrable real random variables on one probability space, pairwise uncorrelated within the row, where rn≥0 is finite. Set Sn=∑k=1rnXn,k and let bn>0 be deterministic. If vn:=bn−2∑k=1rnVar⁡(Xn,k)⟶0, then (Sn−ESn)/bn→0 in L2 and in probability. More precisely, its second moment is vn, and its probability of absolute value at least ε>0 is at most vn/ε2. No independence between rows is required.

[F2]

Convergence in probability: For real random variables (Xn) and X on one probability space, write Xn→X in probability when, for every ε>0, P(∣Xn−X∣>ε)⟶0. This is precisely def-convergence-in-measure for the probability measure.

[F3]

Countably many independent copies of a prescribed law exist: Assume countable choice and dependent choice. Every probability measure ν on (S,Σ) is the common law of a countable independent family of S-valued random elements.

Counterexample

Given: The construction and assumptions above.

1.1F3F1givenalgebra

Under countable choice and dependent choice take IID fair signs using the countable-copy theorem. A row consisting of one random entry and constants is independent: any finite intersection of coordinate events reduces to the one nonconstant event or is empty. Each entry is centered and square-integrable. Its variance sum is n2, so the row weak law has normalized variance 1, not a quantity tending to zero.

2.1F2step 1.1algebra∎

The sum is exactly Sn=nϵn. Thus P(∣Sn/n∣>1/2)=1 for every n≥1, contradicting the defining requirement for convergence in probability to zero. At n=1 the row has only its one random entry. This is an array witness and asserts no failure of the IID integrable weak law.

CounterexampleConstruction: AI-generatedVerification: AI-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07Open item page →

Summable untruncated variances are not necessary

Statement refuted

It is false that almost-sure convergence of a series of independent centered square-integrable variables forces summability of their untruncated variances. Assume countable choice and dependent choice. Let X1=0 and for n≥2 take independent Xn with P(Xn=n)=P(Xn=−n)=12n2,P(Xn=0)=1−1n2. Then ∑nXn converges absolutely almost surely, although EXn=0 and Var⁡(Xn)=1 for every n≥2.

Facts & Assumptions

[F1]

First Borel-Cantelli lemma for events: Let (An)n∈N be events in a probability space. If ∑n=0∞P(An)<+∞, then P(An i.o.)=0. No independence hypothesis is needed.

[F2]

Coordinate random elements of a countable product are independent: Under the measure of thm-countable-product-of-probability-spaces, the coordinate maps Xn(x)=xn have laws μn and are independent.

[F3]

Assuming countable and dependent choice, countable products of arbitrary probability spaces: Assume countable choice and dependent choice. For probability spaces (En,En,μn)n∈N there is a unique probability measure μ on CN such that, for every finite F, its F-coordinate marginal is ⨂n∈Fμn.

[F4]

The p-series for a real exponent p converges exactly when p is greater than one: For every real p, ∑k≥11kp converges⟺p>1.

[F5]

Almost-sure convergence of a random series: For real random variables (Xn)n≥1, the series ∑n≥1Xn converges almost surely if its partial sums Sn converge to a finite real limit on an event of probability one, as in def-almost-sure-convergence-of-random-variables. With S0=0 from def-partial-sums-and-sample-means, its convergence event is C=⋂r≥1⋃N≥1⋂j≥i≥N{∣Sj−Si∣<1/r}. This is exactly the real Cauchy condition, with the indexing of thm-series-cauchy-criterion shifted by one. Measurable arithmetic makes every event in this countable expression measurable. For any fixed m, the union over N may be restricted to N≥m; then each difference uses only Xm+1,Xm+2,…. Thus C is in the tail sigma-algebra, without assuming independence. Under independence, cor-almost-sure-convergence-of-an-independent-series-is-a-zero-one-event gives P(C)∈{0,1}. Set S=lim⁡nSn on C and S=0 off C. The functions 1CSn converge everywhere to S, so thm-sequential-suprema-infima-limsup-liminf-and-pointwise-limits-are-measurable and thm-arithmetic-and-lattice-operations-preserve-measurability make S measurable. For Borel sets Bn, the event {Xn∈Bn infinitely often}=⋂m⋃n≥m{Xn∈Bn} is likewise tail measurable. Changing finitely many summands adds an eventually constant finite difference to Sn; divided by deterministic cn>0 tending to infinity that difference tends to zero, so the normalized limsup is unchanged. The sign of the unnormalized limsup need not be unchanged: the all-zero sequence has limsup zero, while changing its first term to 1 makes the limsup of partial sums equal to 1.

Counterexample

Given: The construction and assumptions above.

1.1F3F2givenalgebra

Under countable choice and dependent choice take the countable product of these finite probability spaces. The specified masses are nonnegative and sum to one; its independent coordinates have the desired laws. For n≥2, direct finite expectation gives EXn=0 and EXn2=n2(1/n2)=1, hence variance 1. The first coordinate is zero.

2.1F4F1F5step 1.1algebra∎

The sum ∑n≥2P(Xn≠0)=∑n≥2n−2 is finite. The first Borel–Cantelli lemma gives only finitely many nonzero terms almost surely. On that event the absolute sum is a finite sum of finite numbers, hence finite, and the original partial sums converge. But their untruncated variance sum is ∑n≥21=∞. The example has no uniform bound on all summands.

CounterexampleConstruction: AI-adaptedVerification: AI-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07Open item page →

Cauchy averages admit no deterministic weak centering

Statement refuted

Assume countable choice and dependent choice. For IID real variables with density f(x)=1/[π(1+x2)] on R, there is no deterministic real sequence (μn) for which Sn/n−μn→0 in probability, where Sn=∑k=1nXk. Thus IID alone cannot guarantee a weak law even with varying deterministic centering.

Facts & Assumptions

[F1]

Exact tail criterion for a truncated-centered IID weak law: For IID real random variables (Xn)n≥1 and Sn=∑k=1nXk, there exist deterministic real constants (μn) with Sn/n−μn→0 in probability if and only if nP(∣X1∣>n)⟶0. When this condition holds, μn=E[X11{∣X1∣≤n}] works. Neither existence of an untruncated mean nor convergence of (μn) is asserted.

[F2]

Countably many independent copies of a prescribed law exist: Assume countable choice and dependent choice. Every probability measure ν on (S,Σ) is the common law of a countable independent family of S-valued random elements.

[F3]

Law or distribution of a random element: Let X:(Ω,F,P)→(S,Σ) be a random element. Its law or distribution is the set function PX:Σ→[0,+∞],PX(B):=P(X−1(B)). Thus the law of X records the probability of each measurable target set by pulling it back to an event in the original probability space.

[F4]

Probability laws correspond to distribution functions: Assume the Axiom of Countable Choice. 1. Let X be a real random variable, let PX be its law, and let FX(x)=P(X≤x). Then FX is nondecreasing and right-continuous, satisfies lim⁡x→−∞FX(x)=0,lim⁡x→+∞FX(x)=1, and obeys PX((a,b])=FX(b)−FX(a)(a<b). 2. Conversely, if F:R→R is nondecreasing and right-continuous with lim⁡x→−∞F(x)=0,lim⁡x→+∞F(x)=1, then there is a unique Borel probability measure μ on R such that μ((a,b])=F(b)−F(a)(a<b), equivalently F(x)=μ((−∞,x])(x∈R).

Counterexample

Given: The construction and assumptions above.

1.1F3F2givenalgebraF4

The nonnegative density has total integral [arctan⁡x/π]−∞∞=1 and F(x)=1/2+arctan⁡(x)/π is nondecreasing and continuous with limits zero and one. The distribution-function correspondence therefore supplies its Borel probability law; the fundamental theorem of calculus identifies its density as f. Under countable choice and dependent choice, construct IID copies with that law. Symmetry of the density gives P(∣X1∣>n)=(2/π)∫n∞(1+x2)−1 dx.

2.1F1step 1.1algebra∎

For x≥n≥1, x−2/(1+n−2)≤(1+x2)−1≤x−2. Integrating and multiplying by n gives 2/[π(1+n−2)]≤nP(∣X1∣>n)≤2/π. Thus this tail quantity tends to 2/π, not zero. Necessity in the truncated-centering criterion rules out every deterministic centering sequence.

ExampleConstruction: AI-adaptedVerification: AI-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07Open item page →

An infinite-mean law requiring diverging centering

Example

Assume countable choice and dependent choice. Let X≥e have survival function P(X>x)=1/(xlog⁡x) for x≥e, with an atom of mass 1−1/e at e. For IID copies (Xk), the untruncated mean is infinite but Sn/n−μn⟶0in probability,μn=e+log⁡log⁡n−1log⁡n(n≥e). Here μn=E[X1{X≤n}]; for integer n<e set μn=0. More generally, the survival family 1/[x(log⁡x)α] for x≥e, α≥0, has infinite second moment for every α, finite first moment exactly for α>1, and admits deterministic weak-law centering exactly for α>0.

Facts & Assumptions

[F1]

Exact tail criterion for a truncated-centered IID weak law: For IID real random variables (Xn)n≥1 and Sn=∑k=1nXk, there exist deterministic real constants (μn) with Sn/n−μn→0 in probability if and only if nP(∣X1∣>n)⟶0. When this condition holds, μn=E[X11{∣X1∣≤n}] works. Neither existence of an untruncated mean nor convergence of (μn) is asserted.

[F2]

Countably many independent copies of a prescribed law exist: Assume countable choice and dependent choice. Every probability measure ν on (S,Σ) is the common law of a countable independent family of S-valued random elements.

[F3]

Layer-cake formulas for random variables: Let (Ω,F,P) be a probability space. 1. If X:Ω→[0,+∞] is measurable, then E[X]=∫0∞P(X>t) dt, where the right-hand side may be +∞. 2. If X is an integrable real random variable, then E[X]=∫0∞P(X>t) dt−∫0∞P(X<−t) dt.

[F4]

Probability laws correspond to distribution functions: Assume the Axiom of Countable Choice. 1. Let X be a real random variable, let PX be its law, and let FX(x)=P(X≤x). Then FX is nondecreasing and right-continuous, satisfies lim⁡x→−∞FX(x)=0,lim⁡x→+∞FX(x)=1, and obeys PX((a,b])=FX(b)−FX(a)(a<b). 2. Conversely, if F:R→R is nondecreasing and right-continuous with lim⁡x→−∞F(x)=0,lim⁡x→+∞F(x)=1, then there is a unique Borel probability measure μ on R such that μ((a,b])=F(b)−F(a)(a<b), equivalently F(x)=μ((−∞,x])(x∈R).

Verification

Given: The construction and assumptions above.

1.1F4F2givenalgebra

Define F(x)=0 for x<e and F(x)=1−1/[x(log⁡x)α] for x≥e, where α≥0. It is nondecreasing and right-continuous with limits zero and one at the two infinities. Its jump at e is 1−1/e. The distribution-function theorem constructs its Borel probability law (using countable choice); under countable choice and dependent choice the countable-copy result constructs IID variables with it.

2.1F3step 1.1algebra

Layer cake gives EX=e+∫e∞[x(log⁡x)α]−1 dx=e+∫1∞u−α du. This is finite exactly for α>1, when it equals e+1/(α−1). Applying layer cake to X2 and substituting t=x2 gives EX2=e2+2∫e∞(log⁡x)−α dx=∞: eventually (log⁡x)α≤x, so the last integrand dominates 1/x. The comparison follows from uα≤eu for large u, for example by an exponential-series term of integer degree greater than α.

2.2F1step 1.1algebra

For n≥e the tail quantity is nP(X>n)=(log⁡n)−α. It tends to zero exactly for α>0, whereas for α=0 it equals one. Both directions of the truncated-centering criterion therefore give exactly the asserted centering range, even in the infinite-mean cases 0<α≤1.

3.1F3step 2.1step 2.2algebra∎

For α=1 use the pointwise identity min⁡(X,n)=X1{X≤n}+n1{X>n}. Layer cake for the bounded minimum gives μn=∫0nP(X>t) dt−nP(X>n)=e+log⁡log⁡n−1/log⁡n for real n≥e. At n=e this is e−1, exactly the contribution of the atom; below e the zero truncation is zero. These finite centers work by the preceding step, although EX=∞ and μn∼log⁡log⁡n→∞.

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