TheoremBase

Proof

Preliminaries. Write EK=∑k=0Kμk/k!E_K=\sum_{k=0}^{K}\mu^{k}/k! for K∈N0K\in\mathbb{N}_0 and E−1=E−2=0E_{-1}=E_{-2}=0. By The Real Exponential Function, EK→exp⁡(μ)E_K\to\exp(\mu) as K→∞K\to\infty (the partial sums of the defining series converge to exp⁡(μ)\exp(\mu)), and hence also EK−1→exp⁡(μ)E_{K-1}\to\exp(\mu) and EK−2→exp⁡(μ)E_{K-2}\to\exp(\mu) as K→∞K\to\infty: for ε>0\varepsilon>0, if ∣EL−exp⁡(μ)∣<ε|E_L-\exp(\mu)|<\varepsilon for all L≥L0L\ge L_0, then ∣EK−1−exp⁡(μ)∣<ε|E_{K-1}-\exp(\mu)|<\varepsilon and ∣EK−2−exp⁡(μ)∣<ε|E_{K-2}-\exp(\mu)|<\varepsilon for all K≥L0+2K\ge L_0+2, which is the definition of the limit. By claim 2 of Basic Properties of the Exponential Function, exp⁡(−μ)exp⁡(μ)=1\exp(-\mu)\exp(\mu)=1 and exp⁡(−μ)>0\exp(-\mu)>0. Since every term μk/k!\mu^{k}/k! is positive, EKE_K is nondecreasing in KK and μk/k!≤EK\mu^{k}/k!\le E_K for k≤Kk\le K; moreover EK≤exp⁡(μ)E_K\le\exp(\mu), by claim 1 of Order Properties of Limits of Real Sequences applied to the constant sequence with value EKE_K (which converges to EKE_K) and the sequence (EL)L≥K(E_L)_{L\ge K}, which dominates it termwise and converges to exp⁡(μ)\exp(\mu) (a tail of a convergent sequence converges to the same limit, by the argument just given for EK−1E_{K-1}). Hence 0<pμ(k)≤exp⁡(−μ)exp⁡(μ)=10<p_\mu(k)\le\exp(-\mu)\exp(\mu)=1 for k∈N0k\in\mathbb{N}_0, so pμp_\mu takes values in [0,1][0,1] and {pμ>0}=N0\{p_\mu>0\}=\mathbb{N}_0. Finally, each singleton {k}=⋂j∈N(k−1/j,k+1/j)\{k\}=\bigcap_{j\in\mathbb{N}}(k-1/j,k+1/j) is a Borel set (a countable intersection of open intervals), and by Poisson Distribution, Pμ({k})=exp⁡(−μ)∑j∈N0∩{k}μj/j!=exp⁡(−μ)μk/k!=pμ(k)P_\mu(\{k\})=\exp(-\mu)\sum_{j\in\mathbb{N}_0\cap\{k\}}\mu^{j}/j!=\exp(-\mu)\mu^{k}/k!=p_\mu(k) for k∈N0k\in\mathbb{N}_0, as asserted in the statement.

(P) Let f:R→[0,∞)f:\mathbb{R}\to[0,\infty) vanish on R∖N0\mathbb{R}\setminus\mathbb{N}_0, suppose the partial sums sK=∑k=0Kf(k)s_K=\sum_{k=0}^{K}f(k) converge to a real number ss, and let AA be a set with N0⊆A⊆R\mathbb{N}_0\subseteq A\subseteq\mathbb{R}. Then the sum of ff over AA equals ss (note s≥0s\ge0: each sK≥0s_K\ge0, so claim 1 of Order Properties of Limits of Real Sequences with the constant sequence 00 gives s≥0s\ge0). Indeed, for a finite set F⊆AF\subseteq A, either F∩N0=∅F\cap\mathbb{N}_0=\emptyset and ∑x∈Ff(x)=0≤s\sum_{x\in F}f(x)=0\le s (if F≠∅F\ne\emptyset every term vanishes, so the sum is a sum of zeros over [∣F∣][|F|] along an enumeration by Sum over a Finite Index Set, hence 00 by Finite Sum Notation in a Field; if F=∅F=\emptyset the empty-sum convention applies), or K=max⁡(F∩N0)K=\max(F\cap\mathbb{N}_0) exists and ∑x∈Ff(x)=∑x∈F∩N0f(x)≤sK≤s\sum_{x\in F}f(x)=\sum_{x\in F\cap\mathbb{N}_0}f(x)\le s_K\le s, using claims 4 and 3 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set (terms vanishing off F∩N0F\cap\mathbb{N}_0; F∩N0⊆{0,…,K}F\cap\mathbb{N}_0\subseteq\{0,\dots,K\} and the omitted terms are nonnegative, the case F∩N0={0,…,K}F\cap\mathbb{N}_0=\{0,\dots,K\} being an equality) and then claim 1 of Order Properties of Limits of Real Sequences applied to the constant sequence sKs_K and the nondecreasing sequence (sL)L≥K(s_L)_{L\ge K}, which converges to ss as a tail of a convergent sequence (by the argument given for EK−1E_{K-1} in the preliminaries). So ss is an upper bound of the finite sums. Conversely each sKs_K is itself a finite sum (over F={0,…,K}⊆AF=\{0,\dots,K\}\subseteq A), so any upper bound bb satisfies b≥sKb\ge s_K for all KK, whence b≥sb\ge s by the same claim. Thus ss is the least upper bound.

Claim 1. Apply (P) to f=pμf=p_\mu and A=RA=\mathbb{R}: sK=exp⁡(−μ)EK→exp⁡(−μ)exp⁡(μ)=1s_K=\exp(-\mu)E_K\to\exp(-\mu)\exp(\mu)=1 by claim 2 of Arithmetic of Limits of Real Sequences. So ∑x∈Rpμ(x)=1\sum_{x\in\mathbb{R}}p_\mu(x)=1, and pμp_\mu is a discrete probability mass function by Discrete Probability Mass Function on Euclidean Space; the identities pμ(k)=Pμ({k})p_\mu(k)=P_\mu(\{k\}) and {pμ>0}=N0\{p_\mu>0\}=\mathbb{N}_0 were shown in the preliminaries.

Claim 2. Let k∈N0k\in\mathbb{N}_0. If k≥1k\ge1, then k!=k⋅(k−1)!k!=k\cdot(k-1)! by Factorial of a Natural Number (with 0!=10!=1 when k=1k=1) and μk=μ⋅μk−1\mu^{k}=\mu\cdot\mu^{k-1}, so

pμ(k−1)pμ(k)=μk−1/(k−1)!μk/k!=kμ.\frac{p_\mu(k-1)}{p_\mu(k)}=\frac{\mu^{k-1}/(k-1)!}{\mu^{k}/k!}=\frac{k}{\mu}.

If k=0k=0, then k−1=−1∉N0k-1=-1\notin\mathbb{N}_0, so pμ(k−1)=0=k/μp_\mu(k-1)=0=k/\mu. In both cases ρpμ,a,w(k)=w1(1−pμ(k−a1)/pμ(k))=w1(1−k/μ)\rho_{p_\mu,a,w}(k)=w_1\bigl(1-p_\mu(k-a_1)/p_\mu(k)\bigr)=w_1(1-k/\mu) by Move Score of a Discrete Probability Mass Function. Finally k+a1=k+1∈N⊆N0k+a_1=k+1\in\mathbb{N}\subseteq\mathbb{N}_0 for every k∈N0k\in\mathbb{N}_0 by Natural Numbers, so no k∈N0k\in\mathbb{N}_0 has k+a1∉N0k+a_1\notin\mathbb{N}_0.

Claim 3. By Move Information of a Discrete Probability Mass Function and claim 2, J(pμ;a,w)\mathsf{J}(p_\mu;a,w) is the sum over N0\mathbb{N}_0 of f(k)=pμ(k) w12(1−k/μ)2=w12μ2 pμ(k)(k−μ)2f(k)=p_\mu(k)\,w_1^{2}(1-k/\mu)^{2}=\frac{w_1^{2}}{\mu^{2}}\,p_\mu(k)(k-\mu)^{2}, and we extend ff by 00 to R∖N0\mathbb{R}\setminus\mathbb{N}_0; by (P) with A=N0A=\mathbb{N}_0 it suffices to show that the partial sums ∑k=0Kpμ(k)(k−μ)2\sum_{k=0}^{K}p_\mu(k)(k-\mu)^{2} converge to μ\mu. Using (k−μ)2=k(k−1)+k−2μk+μ2(k-\mu)^{2}=k(k-1)+k-2\mu k+\mu^{2} and, for k≥1k\ge1, k μk/k!=μ μk−1/(k−1)!k\,\mu^{k}/k!=\mu\,\mu^{k-1}/(k-1)!, and for k≥2k\ge2, k(k−1)μk/k!=μ2μk−2/(k−2)!k(k-1)\mu^{k}/k!=\mu^{2}\mu^{k-2}/(k-2)! (the terms with k=0k=0, respectively k≤1k\le1, vanish),

∑k=0Kkμkk!=μEK−1,∑k=0Kk(k−1)μkk!=μ2EK−2,\sum_{k=0}^{K}k\frac{\mu^{k}}{k!}=\mu E_{K-1},\qquad\sum_{k=0}^{K}k(k-1)\frac{\mu^{k}}{k!}=\mu^{2}E_{K-2},

so that

∑k=0Kpμ(k)(k−μ)2=exp⁡(−μ)(μ2EK−2+μEK−1−2μ2EK−1+μ2EK).\sum_{k=0}^{K}p_\mu(k)(k-\mu)^{2}=\exp(-\mu)\bigl(\mu^{2}E_{K-2}+\mu E_{K-1}-2\mu^{2}E_{K-1}+\mu^{2}E_K\bigr).

By the preliminaries and claims 1 and 3 of Arithmetic of Limits of Real Sequences, the right side converges to exp⁡(−μ)exp⁡(μ)(μ2+μ−2μ2+μ2)=μ\exp(-\mu)\exp(\mu)(\mu^{2}+\mu-2\mu^{2}+\mu^{2})=\mu; multiplying by the constant w12/μ2w_1^{2}/\mu^{2} (claim 3 there), the partial sums of ff converge to w12/μw_1^{2}/\mu. Hence J(pμ;a,w)=w12μ2⋅μ=w12μ\mathsf{J}(p_\mu;a,w)=\frac{w_1^{2}}{\mu^{2}}\cdot\mu=\frac{w_1^{2}}{\mu}. ■\blacksquare

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