Preliminaries. By Factorial of a Natural Number, k!=k(k−1)! for k≥1, and for k≥m, k!/(k−m)!=∏i=1m(k−m+i) (induction on m, peeling the top factor). Hence for k≥m, pμ(k−m)/pμ(k)=μk−mk!/((k−m)!μk)=∏i=1m(k−m+i)/μ, and for k<m the numerator pμ(k−m) vanishes (k−m∈/N0), which justifies the two displayed forms of ϱ. Sums of nonnegative functions over N0 are least upper bounds of finite partial sums (Sum of a Nonnegative Function over an Arbitrary Set); a reindexing k↦k−m along the bijection from {k≥m} onto N0 maps finite subsets onto finite subsets and preserves finite sums (claim 2 of Properties of a Sum over a Finite Index Set), hence preserves the sum over the set; and terms equal to 0 may be dropped, since every finite partial sum over F⊆N0 equals the partial sum over F∩{k≥m} (claims 3 and 4 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set), so the two families of finite partial sums, and hence their least upper bounds, coincide. Let (Ω,F,P) be a probability space carrying a random variable K with the Poisson distribution with parameter μ (it exists by Existence of Independent Sequences with Prescribed Distributions); for every measurable g:R→[0,∞), claim 1 of Series Formula, Exponential Moments, and Chernoff Tail Bounds for the Poisson Distribution gives E[g(K)]=∑k∈N0pμ(k)g(k), and for every natural number j≥1, claim (a) of Factorial Moments and Moments of Every Order of the Poisson Distribution gives that the falling factorial Kj=∏q=0j−1(K−q) is integrable with E[Kj]=μj; put k0=1. Note that kj≥0 for all k∈N0 (for k<j a factor vanishes), so the series formula applies to it, and kj+1=kj(k−j).
Step 1: claim 1. By Move Score of a Discrete Probability Mass Function, ρpμ,a,w(k)=w1(1−pμ(k−m)/pμ(k))=w1(1−ϱ(k)) on the support N0; and k+m∈N0 trivially.
Step 2: claim 2. Dropping the vanishing terms k<m and reindexing, ∑k∈N0pμ(k)ϱ(k)=∑k≥mpμ(k−m)=∑n∈N0pμ(n)=1, the last equality because pμ is a probability mass function with support N0.
Step 3: claim 3. (a) A falling-factorial expansion. For natural numbers ℓ≥0 and 0≤j≤ℓ put cℓ,j=(ℓ!)2/((j!)2(ℓ−j)!), and cℓ,j=0 for j<0 or j>ℓ. We claim that for every ℓ≥0 and every n∈N0,
i=1∏ℓ(n+i)=j=0∑ℓcℓ,jnj.(3.1)
Induction on ℓ: for ℓ=0 both sides equal 1. Assume (3.1) for ℓ. Since (n+ℓ+1)nj=nj(n−j)+(j+ℓ+1)nj=nj+1+(j+ℓ+1)nj, and shifting the summation index in the first resulting sum by one (Invariance of Finite Sums and Products under Reindexing by a Permutation after extending the range with the vanishing coefficients cℓ,−1=cℓ,ℓ+1=0),
i=1∏ℓ+1(n+i)=(n+ℓ+1)j=0∑ℓcℓ,jnj=j=0∑ℓ+1(cℓ,j−1+(j+ℓ+1)cℓ,j)nj.
For 1≤j≤ℓ, using (ℓ+1−j)!=(ℓ+1−j)(ℓ−j)! and (j!)2=j2((j−1)!)2,
cℓ,j−1+(j+ℓ+1)cℓ,j=(j!)2(ℓ+1−j)!(ℓ!)2(j2+(j+ℓ+1)(ℓ+1−j))=(j!)2(ℓ+1−j)!(ℓ!)2(ℓ+1)2=cℓ+1,j;
for j=0 the left side is (ℓ+1)cℓ,0=(ℓ+1)ℓ!=(ℓ+1)!=cℓ+1,0, and for j=ℓ+1 it is cℓ,ℓ=1=cℓ+1,ℓ+1. This proves (3.1) for ℓ+1. Below we use (3.1) with ℓ=m.
(b) The second moment. Dropping the vanishing terms and reindexing k=n+m,
k∈N0∑pμ(k)ϱ(k)2=k≥m∑pμ(k)pμ(k−m)2=n∈N0∑pμ(n)pμ(n+m)pμ(n)=n∈N0∑pμ(n)n!μm(n+m)!=μ−mE[i=1∏m(K+i)],
by the series formula applied to the nonnegative function g(k)=∏i=1m(k+i) (extended by 0 off N0; measurable as it is a polynomial on the Borel set N0). By (3.1), ∏i≤m(K+i)=∑j≤mcm,jKj on the event {K∈N0}, which has probability 1; integrable random variables agreeing off a null event have equal expectations (their difference vanishes off a null set, so its integral is 0 by Lebesgue Integral of a Nonnegative Measurable Function and Simple Function and Its Integral). Hence, by linearity of the expectation (Linearity and Monotonicity of the Lebesgue Integral, all summands being integrable) and the factorial moments,
E[i=1∏m(K+i)]=j=0∑mcm,jμj,sok∑pμ(k)ϱ(k)2=j=0∑mcm,jμj−m=i=0∑mcm,m−iμ−i,
substituting i=m−j (a permutation of the index set, Invariance of Finite Sums and Products under Reindexing by a Permutation), and cm,m−i=(m!)2/(((m−i)!)2i!)=(im)2i!. This is the displayed formula.
(c) The move information and its bounds. By Move Information of a Discrete Probability Mass Function and claim 1, J(pμ;a,w)=∑kpμ(k)w12(1−ϱ(k))2=w12∑kpμ(k)(1−2ϱ(k)+ϱ(k)2). The three sums ∑kpμ(k), ∑kpμ(k)ϱ(k) and ∑kpμ(k)ϱ(k)2 are finite (1, 1 by claim 2, and the finite sum of (b)), so by linearity (the sums being the integrals with respect to the counting measure of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, claims 3 and 4(c), on which claim 2 of Linearity and Monotonicity of the Lebesgue Integral applies), J(pμ;a,w)/w12=1−2+∑i=0m(im)2i!μ−i=∑i=1m(im)2i!μ−i, the i=0 term being 1; for w1=0 the move score vanishes and so does the move information. The i=1 term is m2/μ and the others are nonnegative, giving the lower bound. For the upper bound, (im)2i!=i!1((m−i)!m!)2≤i!m2i, since m!/(m−i)!=∏q=0i−1(m−q)≤mi (claim 5 of Properties of Finite Products); and for i≥2, i!≥2(i−2)!, so with x=m2/μ, ∑i=2mi!xi≤2x2∑i=2m(i−2)!xi−2≤2x2exp(x) by the series for exp (The Real Exponential Function), all terms being nonnegative. Adding the i=1 term gives the upper bound.
Step 4: claim 4. For k≥m, each factor satisfies 0≤(k−m+i)/μ≤k/μ, so ϱ(k)≤(k/μ)m by claim 5 of Properties of Finite Products; for k<m, ϱ(k)=0≤(k/μ)m. Now let x≥0 with m(x+m)≤μ and let k≥μ−x. Then k≥m(x+m)−x≥m2≥m (as mx≥x), so every factor satisfies (k−m+i)/μ≥(k−m)/μ≥(μ−x−m)/μ=1−δ with δ=(x+m)/μ∈[0,1] (as m≥1 gives x+m≤m(x+m)≤μ), hence ϱ(k)≥(1−δ)m by claim 5 of Properties of Finite Products. Finally (1−δ)m≥1−mδ for every natural number m and δ∈[0,1], by induction: it holds for m=1, and multiplying (1−δ)m≥1−mδ by 1−δ≥0 gives (1−δ)m+1≥(1−mδ)(1−δ)=1−(m+1)δ+mδ2≥1−(m+1)δ. With m=m this yields ϱ(k)≥1−m(x+m)/μ. ■