Throughout, write πμ(k)=exp(−μ)μk/k! for nonnegative integers k, with the factorial and the conventions 0!=1 and μ0=1 of the Poisson distribution definition, so that P(K=k)=πμ(k) for every nonnegative integer k by that definition; and write Fp(x)=∏q=0p−1(x−q), with the finite product notation, for real x — a polynomial function of x. Each set {K=k}=K−1({k}) is an event, {k} being a Borel set and K a random variable, so K=⋃k=0∞{K=k}=K−1(N0) is an event by countable-union closure, N0 being the set of nonnegative integers as in the Poisson definition, and P(K)=1 by the final clause of the Poisson distribution definition (a Poisson variable lies in N0 with probability 1). Note that Fp(k)≥0 for every nonnegative integer k: for k≤p−1 the factor k−k occurs and Fp(k)=0, while for k≥p every factor is positive and, by induction on p using the factorial recursion n!=n(n−1)!, Fp(k)=k!/(k−p)!.
Step 1: series formula for nonnegative polynomial moments. Let f be a polynomial function with f(k)≥0 for every nonnegative integer k. Then f(K) is a random variable: a polynomial is sequentially continuous by the algebra of limits of real sequences, so measurability of sequentially continuous functions of measurable maps applies to K. Moreover, writing 1D for the function equal to 1 on a set D and 0 off D,
E[1Kf(K)]=nsup k=0∑nf(k)πμ(k)in [0,∞].
Indeed, the functions hn=∑k=0nf(k)1{K=k} are nonnegative simple functions; grouping the indices k≤n that share a common value c of f, the standard representation of hn assigns to each value c>0 the event ⋃k≤n:f(k)=c{K=k}, whose probability is ∑k≤n:f(k)=cP(K=k) by pairwise disjointness of the {K=k} and finite additivity of P, so the simple-function integral of hn equals ∑k=0nf(k)P(K=k), the value 0 contributing nothing; the hn increase pointwise to 1Kf(K) — at ω∈K with K(ω)=k one has hn(ω)=f(k) for every n≥k, and off K all vanish — and monotone convergence, in its supremum form, gives the display. In particular, taking f≡1: supn∑k=0nπμ(k)=E[1K]=P(K)=1.
Moreover, for any polynomial f, if E[1K∣f(K)∣]<∞ then f(K) is integrable with E[f(K)]=E[1Kf(K)]. Indeed, writing (⋅)+ and (⋅)− for positive and negative parts, one has the pointwise decompositions (f(K))±=(1Kf(K))±+(f(K))±1Kc, where Kc is the complement of K, an event with P(Kc)=1−P(K)=0. The last summand is dominated pointwise by the [0,∞]-valued function equal to ∞ on Kc and 0 elsewhere — the increasing pointwise limit of the simple functions n1Kc, of integral nP(Kc)=0 — so its integral is 0 by monotone convergence and monotonicity. By additivity (clause 1 of the same theorem), E[(f(K))±]=E[(1Kf(K))±], and these are finite, being at most E[1K∣f(K)∣]<∞ by monotonicity, since (1Kf(K))±≤1K∣f(K)∣ pointwise; hence f(K) is integrable and the two expectations agree.
Step 2: clause (a). Apply Step 1 with f=Fp. For every n≥p, the terms with k≤p−1 vanish, and for k≥p one has Fp(k)πμ(k)=exp(−μ)μk/(k−p)!=exp(−μ)μpμk−p/(k−p)!, using Fp(k)=k!/(k−p)! and μk=μpμk−p (which for μ=0 holds by the convention μ0=1). Hence
k=0∑nFp(k)πμ(k)=exp(−μ)μpj=0∑n−pj!μj(j=k−p).
The right-hand partial sums are nondecreasing in n with supremum exp(−μ)μpexp(μ), by the defining series of the real exponential function, and exp(−μ)exp(μ)=exp(0)=1 by clause 1 of the basic properties of the exponential function. Hence E[1KFp(K)]=μp<∞; since Fp(K)≥0 on K, this is also E[1K∣Fp(K)∣], so by Step 1 the random variable Fp(K) is integrable with E[Fp(K)]=μp. This is clause (a).
Step 3: clause (b). For every nonnegative integer k,
kp ≤ (2p)p+2pFp(k):
if k≤2p−1 then kp≤(2p)p and 2pFp(k)≥0; if k≥2p then each factor satisfies k−q≥k−p≥k/2 for q∈{0,…,p−1}, so Fp(k)≥(k/2)p and kp≤2pFp(k). Hence, for every n, termwise,
k=0∑nkpπμ(k) ≤ (2p)pk=0∑nπμ(k)+2pk=0∑nFp(k)πμ(k) ≤ (2p)p+2pμp,
the final step bounding each sum by its supremum, computed in Steps 1 and 2. Taking the supremum over n and using Step 1 with f(x)=xp,
E[1KKp] ≤ (2p)p+2pμp < ∞.
On K one has Kp=∣K∣p=∣Kp∣, so E[1K∣Kp∣]<∞ and, by Step 1, Kp is integrable with E[Kp]=E[1KKp]≤(2p)p+2pμp. This is clause (b).\ □