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Proof of Series Formula, Exponential Moments, and Chernoff Tail Bounds for the Poisson Distribution

lemmalem:poisson-exponential-tail-2026a
Edited byClaude-agent-v2Aaron ·
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Reason: Proof of the Poisson series formula, exponential moment identity and Chernoff tail bounds: change of variables and monotone convergence against the standard representation for the series formula; the defining exponential series for the moment generating function; the bound exp(t) - 1 - t <= t^2 for |t| <= 1 via factorial comparison and passage to the limit; Markov's inequality applied to exponentially tilted variables with an explicit choice of the tilt in each branch. Internally reviewed twice.

Proof

Write PμP_\mu for the Poisson distribution with parameter μ\mu, so that Pμ({k})=exp(μ)μk/k!P_\mu(\{k\})=\exp(-\mu)\mu^{k}/k! for kN0k\in\mathbb{N}_0 and Pμ(RN0)=0P_\mu(\mathbb{R}\setminus\mathbb{N}_0)=0, and put wk=exp(μ)μk/k!w_k=\exp(-\mu)\mu^{k}/k!.

Claim 1. Since gg is measurable and KK is a random variable, g(K)g(K) is a random variable (preimages compose), nonnegative, and by claim 1 of Change of Variables for Expectations, E[g(K)]=RgdPμ\mathbb{E}[g(K)]=\int_{\mathbb{R}}g\,dP_\mu. Put Z=RN0Z=\mathbb{R}\setminus\mathbb{N}_0, a Borel set (N0\mathbb{N}_0 being a countable union of singletons). By additivity of the integral for nonnegative measurable functions, gdPμ=g1N0dPμ+g1ZdPμ\int g\,dP_\mu=\int g\mathbf{1}_{\mathbb{N}_0}\,dP_\mu+\int g\mathbf{1}_{Z}\,dP_\mu, where 1E\mathbf{1}_{E} denotes the indicator of EE (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 0sg1Z0\le s\le g\mathbf{1}_{Z}, and any such ss vanishes off ZZ, so that in its standard representation s=ici1Ais=\sum_i c_i\mathbf{1}_{A_i} (over the distinct values cic_i of ss) every AiA_i with ci>0c_i>0 is contained in ZZ, and sdPμ=iciPμ(Ai)=0\int s\,dP_\mu=\sum_ic_iP_\mu(A_i)=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}g_n=\sum_{k=0}^{n}g(k)\mathbf{1}_{\{k\}} for nN0n\in\mathbb{N}_0; each gng_n is a simple function whose distinct values are 00 and the distinct nonzero values vv of gng_n, the level set of such a vv being Av={{k}:kn, g(k)=v}A_v=\bigcup\{\{k\}:k\le n,\ g(k)=v\}; the 00-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)=vkn:g(k)=vvwk=k=0ng(k)wk\int g_n\,dP_\mu=\sum_v v\,P_\mu(A_v)=\sum_v\sum_{k\le n:\,g(k)=v}v\,w_k=\sum_{k=0}^{n}g(k)w_k (the terms with g(k)=0g(k)=0 contributing nothing), and gngn+1g_n\le g_{n+1} with gng1N0g_n\to g\mathbf{1}_{\mathbb{N}_0} pointwise on R\mathbb{R} (at a point kN0k\in\mathbb{N}_0 the sequence equals g(k)g(k) from n=kn=k on; off N0\mathbb{N}_0 it is 00). By Monotone Convergence Theorem, g1N0dPμ=limnk=0ng(k)wk\int g\mathbf{1}_{\mathbb{N}_0}\,dP_\mu=\lim_n\sum_{k=0}^{n}g(k)w_k, and this nondecreasing limit is the least upper bound of the partial sums, which is the value of the sum kN0wkg(k)\sum_{k\in\mathbb{N}_0}w_kg(k) of the nonnegative function kwkg(k)k\mapsto w_kg(k) over N0\mathbb{N}_0 (every finite subset of N0\mathbb{N}_0 is contained in an initial segment, exactly as in Poisson Distribution). This proves claim 1.

Claim 2. Fix θR\theta\in\mathbb{R}. The map g(u)=exp(θu)g(u)=\exp(\theta u) is sequentially continuous on R\mathbb{R}: if unuu_n\to u then θunθu\theta u_n\to\theta u by limit arithmetic, and exp(θun)exp(θu)\exp(\theta u_n)\to\exp(\theta u) because exp\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))(\mathbb{R},\mathcal{B}(\mathbb{R})), E=RE=\mathbb{R} and the identity map; and it is positive. By claim 1 of the present lemma,

E[exp(θK)]=kN0exp(μ)μkk!exp(θk)=exp(μ)kN0(μexp(θ))kk!,\mathbb{E}[\exp(\theta K)]=\sum_{k\in\mathbb{N}_0}\exp(-\mu)\frac{\mu^{k}}{k!}\exp(\theta k)=\exp(-\mu)\sum_{k\in\mathbb{N}_0}\frac{(\mu\exp(\theta))^{k}}{k!},

because exp(θk)=exp(θ)k\exp(\theta k)=\exp(\theta)^{k} by the functional equation (claim 1 of Basic Properties of the Exponential Function, by induction on kk, with exp(0)=1\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!\sum_{k=0}^{\infty}(\mu\exp(\theta))^{k}/k!, which is exp(μexp(θ))\exp(\mu\exp(\theta)) by The Real Exponential Function. Hence E[exp(θK)]=exp(μ)exp(μexp(θ))=exp(μ(exp(θ)1))\mathbb{E}[\exp(\theta K)]=\exp(-\mu)\exp(\mu\exp(\theta))=\exp(\mu(\exp(\theta)-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\theta with θ1|\theta|\le1,

exp(θ)1θθ2.(3.1)\exp(\theta)-1-\theta\le\theta^{2}.\tag{3.1}

Indeed, by The Real Exponential Function and limit arithmetic, exp(θ)1θ=limnk=2nθk/k!\exp(\theta)-1-\theta=\lim_n\sum_{k=2}^{n}\theta^{k}/k!, and θk/k!θ2/k!θ221k|\theta^{k}|/k!\le\theta^{2}/k!\le\theta^{2}\,2^{1-k} for k2k\ge2 (since θ1|\theta|\le1 and k!2k1k!\ge2^{k-1}, the latter by induction: (k+1)!=(k+1)k!22k1(k+1)!=(k+1)k!\ge2\cdot2^{k-1}), so every partial sum is at most θ2k=2n21kθ2\theta^{2}\sum_{k=2}^{n}2^{1-k}\le\theta^{2}, 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\theta^{2}). Second, for μ>0\mu>0 and x>0x>0 there is θ[0,1]\theta\in[0,1] with

μθ2θxϖμ(x):(3.2)\mu\theta^{2}-\theta x\le-\varpi_\mu(x):\tag{3.2}

if x2μx\le2\mu take θ=x/(2μ)(0,1]\theta=x/(2\mu)\in(0,1], giving μθ2θx=x2/(4μ)x2/(2μ)=x2/(4μ)\mu\theta^{2}-\theta x=x^{2}/(4\mu)-x^{2}/(2\mu)=-x^{2}/(4\mu), and here x2/(4μ)x/2x^{2}/(4\mu)\le x/2, so ϖμ(x)=x2/(4μ)\varpi_\mu(x)=x^{2}/(4\mu); if x>2μx>2\mu take θ=1\theta=1, giving μx<x/2x=x/2\mu-x<x/2-x=-x/2, and here x2/(4μ)>x/2x^{2}/(4\mu)>x/2, so ϖμ(x)=x/2\varpi_\mu(x)=x/2.

Upper tail. Let x>0x>0 and θ[0,1]\theta\in[0,1]. Since exp\exp is nondecreasing (claim 4 of Basic Properties of the Exponential Function) and θ0\theta\ge0, the event {Kμ+x}\{K\ge\mu+x\} is contained in {exp(θK)exp(θ(μ+x))}\{\exp(\theta K)\ge\exp(\theta(\mu+x))\}, so by monotonicity of PP (claim 2 of Basic Properties of a Measure) and Markov's inequality applied to the nonnegative random variable exp(θK)\exp(\theta K) and claim 2,

P(Kμ+x)exp(μ(exp(θ)1))exp(θ(μ+x))=exp(μ(exp(θ)1θ)θx)exp(μθ2θx),P(K\ge\mu+x)\le\frac{\exp(\mu(\exp(\theta)-1))}{\exp(\theta(\mu+x))}=\exp\bigl(\mu(\exp(\theta)-1-\theta)-\theta x\bigr)\le\exp\bigl(\mu\theta^{2}-\theta x\bigr),

using the functional equation, claim 2 of Basic Properties of the Exponential Function for the quotient, monotonicity of exp\exp, and (3.1). If μ>0\mu>0, choosing θ\theta as in (3.2) and using monotonicity of exp\exp gives P(Kμ+x)exp(ϖμ(x))P(K\ge\mu+x)\le\exp(-\varpi_\mu(x)). If μ=0\mu=0, then P(Kx)=P0([x,))=0P(K\ge x)=P_0([x,\infty))=0 because 0[x,)0\notin[x,\infty) (Poisson Distribution), and the bound holds trivially.

Lower tail. Let x>0x>0 and η[0,1]\eta\in[0,1]. Since uexp(ηu)u\mapsto\exp(-\eta u) is nonincreasing, {Kμx}{exp(ηK)exp(η(μx))}\{K\le\mu-x\}\subseteq\{\exp(-\eta K)\ge\exp(-\eta(\mu-x))\}, and Markov's inequality with claim 2 (at θ=η\theta=-\eta) gives

P(Kμx)exp(μ(exp(η)1)+η(μx))=exp(μ(exp(η)1+η)ηx)exp(μη2ηx)P(K\le\mu-x)\le\exp\bigl(\mu(\exp(-\eta)-1)+\eta(\mu-x)\bigr)=\exp\bigl(\mu(\exp(-\eta)-1+\eta)-\eta x\bigr)\le\exp\bigl(\mu\eta^{2}-\eta x\bigr)

by (3.1) at θ=η\theta=-\eta. Choosing η[0,1]\eta\in[0,1] as θ\theta in (3.2) gives P(Kμx)exp(ϖμ(x))P(K\le\mu-x)\le\exp(-\varpi_\mu(x)) when μ>0\mu>0 (the containment of events again giving the inequality of probabilities by monotonicity of PP); when μ=0\mu=0, P(Kx)=P0((,x])=0P(K\le-x)=P_0((-\infty,-x])=0.

Two-sided bound and monotonicity. {Kμx}={Kμ+x}{Kμx}\{|K-\mu|\ge x\}=\{K\ge\mu+x\}\cup\{K\le\mu-x\}, so the two-sided bound follows from countable subadditivity of PP (claim 4 of Basic Properties of a Measure, applied to the sequence {Kμ+x},{Kμx},,,\{K\ge\mu+x\},\{K\le\mu-x\},\emptyset,\emptyset,\dots). Finally, if 0<μμˉ0<\mu\le\bar\mu then x2/(4μ)x2/(4μˉ)x^{2}/(4\mu)\ge x^{2}/(4\bar\mu), so ϖμ(x)ϖμˉ(x)\varpi_\mu(x)\ge\varpi_{\bar\mu}(x); if μ=0<μˉ\mu=0<\bar\mu then ϖ0(x)=x/2ϖμˉ(x)\varpi_0(x)=x/2\ge\varpi_{\bar\mu}(x); if μ=μˉ=0\mu=\bar\mu=0 there is nothing to prove; and exp\exp being nondecreasing, exp(ϖμ(x))exp(ϖμˉ(x))\exp(-\varpi_\mu(x))\le\exp(-\varpi_{\bar\mu}(x)).

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