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The Hoeffding MGF bound for a variable in a unit interval

Statement

Let Y be a measurable real random variable on a probability space with 0≤Y≤1 almost surely. Then, for every λ∈R,

Eexp⁡{λ(Y−EY)}≤exp⁡(λ2/8).

This proof uses only finite product and scalar integral arguments; it does not assume the Axiom of Choice.

Facts & Assumptions

Given: A probability space, a measurable Y with 0≤Y≤1 almost surely, and λ∈R.

[F1]

If X≤W almost surely for integrable real variables, then EX≤EW (Linearity, monotonicity, and the modulus bound for expectation).

[F2]

For 0≤t≤1 and real x,y, exp⁡((1−t)x+ty)≤(1−t)exp⁡(x)+texp⁡(y) (The two-point convexity inequality for the exponential function).

[F3]

For u>0, log⁡ is differentiable and log⁡′(u)=1/u; exp⁡′=exp⁡ (The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t, The exponential function is smooth and (exp⁡)′=exp⁡).

[F5]

If a differentiable function has continuous integrable derivative on a compact interval, the second fundamental theorem evaluates the integral of that derivative by endpoint differences (The second fundamental theorem: if G is differentiable on [a,b] with G′=f and f is integrable, then ∫abf=G(b)−G(a)).

[F7]

A real-valued function is measurable when all strict upper or all strict lower threshold sets are measurable; the exponential is strictly increasing, positive, and inverse to the natural logarithm on positive inputs (Threshold characterisations of real-valued and extended-real-valued measurability, The exponential function is strictly increasing, The exponential is positive and satisfies exp⁡(−x)=1/exp⁡(x), The natural logarithm as the inverse of the exponential function).

[F8]

The exponential addition formula is exp⁡(x+y)=exp⁡(x)exp⁡(y) (The exponential addition formula exp⁡(x+y)=exp⁡(x)exp⁡(y)).

[F9]

Absolute values of measurable real functions are measurable. A statement holding almost surely has a measurable null exceptional set. The probability measure satisfies P(Ω)=1. For nonnegative measurable g, the set function B↦∫Bg dP is a measure; the nonnegative integral is monotone under pointwise order, indicators integrate to their measures, and integrals over null sets vanish. A real measurable function is integrable exactly when its absolute-value integral is finite (Arithmetic and lattice operations preserve measurability whenever they are defined, Measure-null sets and almost-everywhere statements relative to a measure, Probability measures and probability spaces, The indefinite integral of a nonnegative measurable function is a measure, Integral over a measurable subset, Monotonicity and nonnegative homogeneity of the nonnegative integral, The integral of a nonnegative simple function, A nonnegative integral over a null set vanishes, Integrable real and complex functions, and their integrals).

Proof

Given: A probability space, a measurable Y with 0≤Y≤1 almost surely, and λ∈R.

1.1F6F7givenalgebra

Let X be any measurable real random variable. For a<0, {eλX>a} is the whole probability space by [F6]. For a≥0 and λ=0, this set is the whole space if a<1 and empty if a≥1. For a≥0 and λ≠0, it is the whole space when a=0; when a>0, strict increase of the exponential and the inverse relation with log⁡ give {eλX>a}={{X>(log⁡a)/λ},λ>0,{X<(log⁡a)/λ},λ<0. Every set on the right is measurable by [F7]. Thus eλX is measurable by the threshold characterization, with no appeal to a continuous-map Borel measurability result qualified by Countable Choice.

2.1F1F2F9step 1.1given

Let A:={∣Y∣≤1}, measurable by [F9], so P(A)=1. Define ν(B):=∫B∣Y∣ dP; by [F9] this is a measure. Since ∣Y∣1A≤1A, [F9] gives ν(A)≤P(A)=1, while P(Ac)=0 gives ν(Ac)=0. Therefore E∣Y∣=ν(Ω)=ν(A)+ν(Ac)≤1, so Y is integrable by [F9]. Put p:=EY; then [F1] gives p∈[0,1]. The shifted variable Y−p is measurable because {Y−p>a}={Y>a+p} for every real a. Applying step 1.1 to X=Y and X=Y−p establishes measurability of both exponentials. Applying [F2] with endpoints 0,λ gives eλy≤1−y+yeλ for every y∈[0,1]; taking expectations yields EeλY≤1−p+peλ.

3.1givenF3F4F6step 2.1algebra

Define g(λ):=1−p+peλ>0 and ψ(λ):=log⁡g(λ)−pλ. Positivity follows from [F6] and p∈[0,1]. With q(λ):=peλ/g(λ)∈[0,1], [F3]–[F4] give ψ(0)=ψ′(0)=0 and ψ′′(λ)=q(λ)(1−q(λ))∈[0,1/4]. The formula also covers p=0 or p=1, since then g remains positive.

4.1F5step 3.1algebra

The function ψ′′ in step 3.1 is continuous. For λ≥0, integrating twice by [F5] gives ψ(λ)=∫0λ(λ−s)ψ′′(s) ds≤λ2/8. For λ<0, the same endpoint formula written from λ to 0 gives ψ(λ)=∫λ0(s−λ)ψ′′(s) ds≤λ2/8.

5.1F8step 2.1step 4.1algebra∎

By step 2.1 and the exponential addition formula [F8], Eeλ(Y−p)=e−λpEeλY≤e−λpg(λ)=eψ(λ); step 4.1 bounds this by eλ2/8. This proves the claim for every real λ, including λ=0.

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