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Bernstein tail bound for independent bounded sums

Statement

Let Z1,…,Zm be independent, integrable, centered real random variables on a probability space, with ∣Zi∣≤b almost surely for a finite b>0. Put Sm=∑i=1mZi and V=∑i=1mE[Zi2]. For every t>0, if V>0 then P(Sm≥t)≤exp⁡ ⁣(−t22(V+bt/3)),P(Sm≤−t)≤exp⁡ ⁣(−t22(V+bt/3)). If V=0, then Sm=0 almost surely.

Facts & Assumptions

Given: A probability space and a finite independent family Z1,…,Zm of integrable real random variables with EZi=0 and ∣Zi∣≤b almost surely, where b>0.

[F1]

Probability measures and probability spaces and Expectation of a nonnegative or integrable random variable: a probability space has total mass one, and expectation of an integrable random variable is its integral against that probability measure.

[F2]

The Lebesgue integral is linear on L1(μ): the integral is linear on finite sums of integrable functions.

[F3]

The real exponential function and the number e by a power series: exp⁡(x)=∑k≥0xk/k! for every real x.

[F4]

The exponential addition formula exp⁡(x+y)=exp⁡(x)exp⁡(y): exp⁡(x+y)=exp⁡(x)exp⁡(y) for real x,y.

[F5]

Expectations factor over finite products of independent random variables: expectations of finite products of nonnegative measurable functions of independent variables factor.

[F6]

Markov's inequality for random variables: for nonnegative Y and a>0, P(Y≥a)≤E[Y]/a.

[F7]

A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere: a nonnegative random variable with expectation zero vanishes almost surely.

[F8]

Independent random elements: independence means factorization of probabilities of finite measurable-coordinate events.

[F9]

The exponential function is strictly increasing: the exponential is continuous and strictly increasing.

[F10]

Arithmetic and lattice operations preserve measurability whenever they are defined and Composition with a Borel measurable outer map preserves measurability: scalar arithmetic preserves measurability, and composing a measurable real-valued map with a Borel map preserves measurability.

Proof

1.1F1F2F3F9F10given

If m=0, then Sm=V=0, so the zero-variance clause holds. Suppose m≥1, fix one centered variable Z with ∣Z∣≤b, and let σ2=E[Z2]. For every integer k≥2, the power functions are Borel and x↦eλx is continuous by [F9], so their compositions with Z are measurable by [F10]; the almost-sure bound gives integrability of each power. Thus ∣E[Zk]∣≤E[∣Z∣k]≤bk−2σ2. For fixed real λ, the exponential series converges uniformly on [−b,b]: its tail is bounded by ∑k>N(∣λ∣b)k/k!→0. Since ∣Z∣≤b almost surely, this uniform convergence and finite linearity [F2] permit termwise expectation in [F3], and the centered first-order term vanishes.

2.1F3F9F10step 1.1algebra

For k≥2, k!≥2⋅3k−2, by induction from 2!=2 and the fact that each next factor is at least 3. If ∣λ∣b<3, [F3] and step 1.1 therefore give EeλZ≤1+σ2∑k≥2∣λ∣kbk−2k!≤1+λ2σ22(1−∣λ∣b/3)≤exp⁡ ⁣(λ2σ22(1−∣λ∣b/3)), where the last inequality follows from 1+x≤ex for x≥0, which follows termwise from [F3].

3.1F4F5F8F9F10step 2.1

For 0<λ<3/b, repeated use of [F4] gives eλSm=∏i=1meλZi. Each Zi is measurable, scalar multiplication preserves measurability by [F10], and x↦ex is Borel by [F9], so the factors are measurable by composition. They are nonnegative functions of the independent variables, so [F5] and step 2.1 yield EeλSm=∏i=1mEeλZi≤exp⁡ ⁣(λ2V2(1−λb/3)).

4.1F3F6F9F10step 3.1algebra

If V>0, take λ=t/(V+bt/3); then 0<λb/3=bt/(3V+bt)<1. The finite sum Sm and its threshold event are measurable by [F10]. Since [F9] makes ex increasing, on {Sm≥t} one has eλSm≥eλt. Markov [F6] and step 3.1 give P(Sm≥t)≤exp⁡ ⁣(λ2V2(1−λb/3)−λt)=exp⁡ ⁣(−t22(V+bt/3)).

5.1F7givenstep 4.1∎

Applying step 4.1 to −Z1,…,−Zm gives the lower-tail bound, since this family remains independent, centered, bounded by b, and has the same total second moment V. If V=0, each nonnegative Zi2 has expectation zero, so [F7] makes every Zi=0 almost surely; their finite sum is then zero almost surely.

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