Write Pμ for the Poisson distribution with parameter μ, so that Pμ({k})=exp(−μ)μk/k! for k∈N0 and Pμ(R∖N0)=0, and put wk=exp(−μ)μk/k!.
Claim 1. Since g is measurable and K is a random variable, g(K) is a random variable (preimages compose), nonnegative, and by claim 1 of Change of Variables for Expectations, E[g(K)]=∫RgdPμ. Put Z=R∖N0, a Borel set (N0 being a countable union of singletons). By additivity of the integral for nonnegative measurable functions, ∫gdPμ=∫g1N0dPμ+∫g1ZdPμ, where 1E denotes the indicator of E (a measurable function by claim 1 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, products being measurable by claim 3 there). The second integral vanishes: by Lebesgue Integral of a Nonnegative Measurable Function it is the least upper bound of the integrals of simple functions 0≤s≤g1Z, and any such s vanishes off Z, so that in its standard representation s=∑ici1Ai (over the distinct values ci of s) every Ai with ci>0 is contained in Z, and ∫sdPμ=∑iciPμ(Ai)=0 by monotonicity of the measure (claim 2 of Basic Properties of a Measure). For the first integral let gn=∑k=0ng(k)1{k} for n∈N0; each gn is a simple function whose distinct values are 0 and the distinct nonzero values v of gn, the level set of such a v being Av=⋃{{k}:k≤n, g(k)=v}; the 0-term of the standard representation contributes nothing to the integral, so by Simple Function and Its Integral and finite additivity (claim 1 of Basic Properties of a Measure) ∫gndPμ=∑vvPμ(Av)=∑v∑k≤n:g(k)=vvwk=∑k=0ng(k)wk (the terms with g(k)=0 contributing nothing), and gn≤gn+1 with gn→g1N0 pointwise on R (at a point k∈N0 the sequence equals g(k) from n=k on; off N0 it is 0). By Monotone Convergence Theorem, ∫g1N0dPμ=limn∑k=0ng(k)wk, and this nondecreasing limit is the least upper bound of the partial sums, which is the value of the sum ∑k∈N0wkg(k) of the nonnegative function k↦wkg(k) over N0 (every finite subset of N0 is contained in an initial segment, exactly as in Poisson Distribution). This proves claim 1.
Claim 2. Fix θ∈R. The map g(u)=exp(θu) is sequentially continuous on R: if un→u then θun→θu by limit arithmetic, and exp(θun)→exp(θu) because exp is differentiable everywhere (claim 3 of Basic Properties of the Exponential Function), hence continuous, hence sequentially continuous; so it is Borel measurable by Sequentially Continuous Functions of Measurable Euclidean Maps are Measurable applied with the measurable space (R,B(R)), E=R and the identity map; and it is positive. By claim 1 of the present lemma,
E[exp(θK)]=k∈N0∑exp(−μ)k!μkexp(θk)=exp(−μ)k∈N0∑k!(μexp(θ))k,
because exp(θk)=exp(θ)k by the functional equation (claim 1 of Basic Properties of the Exponential Function, by induction on k, with exp(0)=1) and because a nonnegative constant factor may be taken out of a sum of nonnegative terms (the least upper bound of the scaled partial sums being the scaled least upper bound). The last sum has nonnegative terms, so it equals the limit of the partial sums of the series ∑k=0∞(μexp(θ))k/k!, which is exp(μexp(θ)) by The Real Exponential Function. Hence E[exp(θK)]=exp(−μ)exp(μexp(θ))=exp(μ(exp(θ)−1)) by the functional equation, a finite number; a nonnegative random variable with finite expectation is integrable.
Claim 3. Two elementary inequalities. For real θ with ∣θ∣≤1,
exp(θ)−1−θ≤θ2.(3.1)
Indeed, by The Real Exponential Function and limit arithmetic, exp(θ)−1−θ=limn∑k=2nθk/k!, and ∣θk∣/k!≤θ2/k!≤θ221−k for k≥2 (since ∣θ∣≤1 and k!≥2k−1, the latter by induction: (k+1)!=(k+1)k!≥2⋅2k−1), so every partial sum is at most θ2∑k=2n21−k≤θ2, and the bound passes to the limit by the comparison claim 1 of Order Properties of Limits of Real Sequences (against the constant sequence θ2). Second, for μ>0 and x>0 there is θ∈[0,1] with
μθ2−θx≤−ϖμ(x):(3.2)
if x≤2μ take θ=x/(2μ)∈(0,1], giving μθ2−θx=x2/(4μ)−x2/(2μ)=−x2/(4μ), and here x2/(4μ)≤x/2, so ϖμ(x)=x2/(4μ); if x>2μ take θ=1, giving μ−x<x/2−x=−x/2, and here x2/(4μ)>x/2, so ϖμ(x)=x/2.
Upper tail. Let x>0 and θ∈[0,1]. Since exp is nondecreasing (claim 4 of Basic Properties of the Exponential Function) and θ≥0, the event {K≥μ+x} is contained in {exp(θK)≥exp(θ(μ+x))}, so by monotonicity of P (claim 2 of Basic Properties of a Measure) and Markov's inequality applied to the nonnegative random variable exp(θK) and claim 2,
P(K≥μ+x)≤exp(θ(μ+x))exp(μ(exp(θ)−1))=exp(μ(exp(θ)−1−θ)−θx)≤exp(μθ2−θx),
using the functional equation, claim 2 of Basic Properties of the Exponential Function for the quotient, monotonicity of exp, and (3.1). If μ>0, choosing θ as in (3.2) and using monotonicity of exp gives P(K≥μ+x)≤exp(−ϖμ(x)). If μ=0, then P(K≥x)=P0([x,∞))=0 because 0∈/[x,∞) (Poisson Distribution), and the bound holds trivially.
Lower tail. Let x>0 and η∈[0,1]. Since u↦exp(−ηu) is nonincreasing, {K≤μ−x}⊆{exp(−ηK)≥exp(−η(μ−x))}, and Markov's inequality with claim 2 (at θ=−η) gives
P(K≤μ−x)≤exp(μ(exp(−η)−1)+η(μ−x))=exp(μ(exp(−η)−1+η)−ηx)≤exp(μη2−ηx)
by (3.1) at θ=−η. Choosing η∈[0,1] as θ in (3.2) gives P(K≤μ−x)≤exp(−ϖμ(x)) when μ>0 (the containment of events again giving the inequality of probabilities by monotonicity of P); when μ=0, P(K≤−x)=P0((−∞,−x])=0.
Two-sided bound and monotonicity. {∣K−μ∣≥x}={K≥μ+x}∪{K≤μ−x}, so the two-sided bound follows from countable subadditivity of P (claim 4 of Basic Properties of a Measure, applied to the sequence {K≥μ+x},{K≤μ−x},∅,∅,…). Finally, if 0<μ≤μˉ then x2/(4μ)≥x2/(4μˉ), so ϖμ(x)≥ϖμˉ(x); if μ=0<μˉ then ϖ0(x)=x/2≥ϖμˉ(x); if μ=μˉ=0 there is nothing to prove; and exp being nondecreasing, exp(−ϖμ(x))≤exp(−ϖμˉ(x)).