TheoremBase

Proof

Preliminaries. By Factorial of a Natural Number, k!=k (k−1)!k!=k\,(k-1)! for k≥1k\ge1, and for k≥mk\ge\mathsf{m}, k!/(k−m)!=∏i=1m(k−m+i)k!/(k-\mathsf{m})!=\prod_{i=1}^{\mathsf{m}}(k-\mathsf{m}+i) (induction on m\mathsf{m}, peeling the top factor). Hence for k≥mk\ge\mathsf{m}, pμ(k−m)/pμ(k)=μk−mk!/((k−m)! μk)=∏i=1m(k−m+i)/μp_\mu(k-\mathsf{m})/p_\mu(k)=\mu^{k-\mathsf{m}}k!/((k-\mathsf{m})!\,\mu^{k})=\prod_{i=1}^{\mathsf{m}}(k-\mathsf{m}+i)/\mu, and for k<mk<\mathsf{m} the numerator pμ(k−m)p_\mu(k-\mathsf{m}) vanishes (k−m∉N0k-\mathsf{m}\notin\mathbb{N}_0), which justifies the two displayed forms of ϱ\varrho. Sums of nonnegative functions over N0\mathbb{N}_0 are least upper bounds of finite partial sums (Sum of a Nonnegative Function over an Arbitrary Set); a reindexing k↦k−mk\mapsto k-\mathsf{m} along the bijection from {k≥m}\{k\ge\mathsf{m}\} onto N0\mathbb{N}_0 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 00 may be dropped, since every finite partial sum over F⊆N0F\subseteq\mathbb{N}_0 equals the partial sum over F∩{k≥m}F\cap\{k\ge\mathsf{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)(\Omega,\mathcal{F},P) be a probability space carrying a random variable KK with the Poisson distribution with parameter μ\mu (it exists by Existence of Independent Sequences with Prescribed Distributions); for every measurable g:R→[0,∞)g:\mathbb{R}\to[0,\infty), claim 1 of Series Formula, Exponential Moments, and Chernoff Tail Bounds for the Poisson Distribution gives E[g(K)]=∑k∈N0pμ(k)g(k)\mathbb{E}[g(K)]=\sum_{k\in\mathbb{N}_0}p_\mu(k)g(k), and for every natural number j≥1j\ge1, 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)K^{\underline{j}}=\prod_{q=0}^{j-1}(K-q) is integrable with E[Kj‾]=μj\mathbb{E}[K^{\underline{j}}]=\mu^{j}; put k0‾=1k^{\underline{0}}=1. Note that kj‾≥0k^{\underline{j}}\ge0 for all k∈N0k\in\mathbb{N}_0 (for k<jk<j a factor vanishes), so the series formula applies to it, and kj+1‾=kj‾(k−j)k^{\underline{j+1}}=k^{\underline{j}}(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))\rho_{p_\mu,a,w}(k)=w_1(1-p_\mu(k-\mathsf{m})/p_\mu(k))=w_1(1-\varrho(k)) on the support N0\mathbb{N}_0; and k+m∈N0k+\mathsf{m}\in\mathbb{N}_0 trivially.

Step 2: claim 2. Dropping the vanishing terms k<mk<\mathsf{m} and reindexing, ∑k∈N0pμ(k)ϱ(k)=∑k≥mpμ(k−m)=∑n∈N0pμ(n)=1\sum_{k\in\mathbb{N}_0}p_\mu(k)\varrho(k)=\sum_{k\ge\mathsf{m}}p_\mu(k-\mathsf{m})=\sum_{n\in\mathbb{N}_0}p_\mu(n)=1, the last equality because pμp_\mu is a probability mass function with support N0\mathbb{N}_0.

Step 3: claim 3. (a) A falling-factorial expansion. For natural numbers ℓ≥0\ell\ge0 and 0≤j≤ℓ0\le j\le\ell put cℓ,j=(ℓ!)2/((j!)2(ℓ−j)!)c_{\ell,j}=(\ell!)^{2}/\bigl((j!)^{2}(\ell-j)!\bigr), and cℓ,j=0c_{\ell,j}=0 for j<0j<0 or j>ℓj>\ell. We claim that for every ℓ≥0\ell\ge0 and every n∈N0n\in\mathbb{N}_0,

∏i=1ℓ(n+i)=∑j=0ℓcℓ,j nj‾.(3.1)\prod_{i=1}^{\ell}(n+i)=\sum_{j=0}^{\ell}c_{\ell,j}\,n^{\underline{j}} .\tag{3.1}

Induction on ℓ\ell: for ℓ=0\ell=0 both sides equal 11. Assume (3.1) for ℓ\ell. Since (n+ℓ+1) nj‾=nj‾(n−j)+(j+ℓ+1)nj‾=nj+1‾+(j+ℓ+1)nj‾(n+\ell+1)\,n^{\underline{j}}=n^{\underline{j}}(n-j)+(j+\ell+1)n^{\underline{j}}=n^{\underline{j+1}}+(j+\ell+1)n^{\underline{j}}, 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=0c_{\ell,-1}=c_{\ell,\ell+1}=0),

∏i=1ℓ+1(n+i)=(n+ℓ+1)∑j=0ℓcℓ,jnj‾=∑j=0ℓ+1(cℓ,j−1+(j+ℓ+1)cℓ,j)nj‾.\prod_{i=1}^{\ell+1}(n+i)=(n+\ell+1)\sum_{j=0}^{\ell}c_{\ell,j}n^{\underline{j}}=\sum_{j=0}^{\ell+1}\bigl(c_{\ell,j-1}+(j+\ell+1)c_{\ell,j}\bigr)n^{\underline{j}} .

For 1≤j≤ℓ1\le j\le\ell, using (ℓ+1−j)!=(ℓ+1−j)(ℓ−j)!(\ell+1-j)!=(\ell+1-j)(\ell-j)! and (j!)2=j2((j−1)!)2(j!)^{2}=j^{2}((j-1)!)^{2},

cℓ,j−1+(j+ℓ+1)cℓ,j=(ℓ!)2(j!)2(ℓ+1−j)!(j2+(j+ℓ+1)(ℓ+1−j))=(ℓ!)2(ℓ+1)2(j!)2(ℓ+1−j)!=cℓ+1,j;c_{\ell,j-1}+(j+\ell+1)c_{\ell,j}=\frac{(\ell!)^{2}}{(j!)^{2}(\ell+1-j)!}\bigl(j^{2}+(j+\ell+1)(\ell+1-j)\bigr)=\frac{(\ell!)^{2}(\ell+1)^{2}}{(j!)^{2}(\ell+1-j)!}=c_{\ell+1,j};

for j=0j=0 the left side is (ℓ+1)cℓ,0=(ℓ+1) ℓ!=(ℓ+1)!=cℓ+1,0(\ell+1)c_{\ell,0}=(\ell+1)\,\ell!=(\ell+1)!=c_{\ell+1,0}, and for j=ℓ+1j=\ell+1 it is cℓ,ℓ=1=cℓ+1,ℓ+1c_{\ell,\ell}=1=c_{\ell+1,\ell+1}. This proves (3.1) for ℓ+1\ell+1. Below we use (3.1) with ℓ=m\ell=\mathsf{m}.

(b) The second moment. Dropping the vanishing terms and reindexing k=n+mk=n+\mathsf{m},

∑k∈N0pμ(k)ϱ(k)2=∑k≥mpμ(k−m)2pμ(k)=∑n∈N0pμ(n)pμ(n)pμ(n+m)=∑n∈N0pμ(n)(n+m)!n! μm=μ−m E[∏i=1m(K+i)],\sum_{k\in\mathbb{N}_0}p_\mu(k)\varrho(k)^{2}=\sum_{k\ge\mathsf{m}}\frac{p_\mu(k-\mathsf{m})^{2}}{p_\mu(k)}=\sum_{n\in\mathbb{N}_0}p_\mu(n)\frac{p_\mu(n)}{p_\mu(n+\mathsf{m})}=\sum_{n\in\mathbb{N}_0}p_\mu(n)\frac{(n+\mathsf{m})!}{n!\,\mu^{\mathsf{m}}}=\mu^{-\mathsf{m}}\,\mathbb{E}\Bigl[\prod_{i=1}^{\mathsf{m}}(K+i)\Bigr],

by the series formula applied to the nonnegative function g(k)=∏i=1m(k+i)g(k)=\prod_{i=1}^{\mathsf{m}}(k+i) (extended by 00 off N0\mathbb{N}_0; measurable as it is a polynomial on the Borel set N0\mathbb{N}_0). By (3.1), ∏i≤m(K+i)=∑j≤mcm,jKj‾\prod_{i\le\mathsf{m}}(K+i)=\sum_{j\le\mathsf{m}}c_{\mathsf{m},j}K^{\underline{j}} on the event {K∈N0}\{K\in\mathbb{N}_0\}, which has probability 11; integrable random variables agreeing off a null event have equal expectations (their difference vanishes off a null set, so its integral is 00 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=1m(K+i)]=∑j=0mcm,jμj,so∑kpμ(k)ϱ(k)2=∑j=0mcm,jμj−m=∑i=0mcm,m−iμ−i,\mathbb{E}\Bigl[\prod_{i=1}^{\mathsf{m}}(K+i)\Bigr]=\sum_{j=0}^{\mathsf{m}}c_{\mathsf{m},j}\mu^{j},\qquad\text{so}\qquad \sum_kp_\mu(k)\varrho(k)^{2}=\sum_{j=0}^{\mathsf{m}}c_{\mathsf{m},j}\mu^{j-\mathsf{m}}=\sum_{i=0}^{\mathsf{m}}c_{\mathsf{m},\mathsf{m}-i}\mu^{-i},

substituting i=m−ji=\mathsf{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!)=(mi)2i!c_{\mathsf{m},\mathsf{m}-i}=(\mathsf{m}!)^{2}/\bigl(((\mathsf{m}-i)!)^{2}i!\bigr)=\binom{\mathsf{m}}{i}^{2}i!. 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)\mathsf{J}(p_\mu;a,w)=\sum_kp_\mu(k)w_1^{2}(1-\varrho(k))^{2}=w_1^{2}\sum_kp_\mu(k)\bigl(1-2\varrho(k)+\varrho(k)^{2}\bigr). The three sums ∑kpμ(k)\sum_kp_\mu(k), ∑kpμ(k)ϱ(k)\sum_kp_\mu(k)\varrho(k) and ∑kpμ(k)ϱ(k)2\sum_kp_\mu(k)\varrho(k)^{2} are finite (11, 11 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(mi)2i!μ−i=∑i=1m(mi)2i!μ−i\mathsf{J}(p_\mu;a,w)/w_1^{2}=1-2+\sum_{i=0}^{\mathsf{m}}\binom{\mathsf{m}}{i}^{2}i!\mu^{-i}=\sum_{i=1}^{\mathsf{m}}\binom{\mathsf{m}}{i}^{2}i!\mu^{-i}, the i=0i=0 term being 11; for w1=0w_1=0 the move score vanishes and so does the move information. The i=1i=1 term is m2/μ\mathsf{m}^{2}/\mu and the others are nonnegative, giving the lower bound. For the upper bound, (mi)2i!=1i!(m!(m−i)!)2≤m2ii!\binom{\mathsf{m}}{i}^{2}i!=\frac{1}{i!}\Bigl(\frac{\mathsf{m}!}{(\mathsf{m}-i)!}\Bigr)^{2}\le\frac{\mathsf{m}^{2i}}{i!}, since m!/(m−i)!=∏q=0i−1(m−q)≤mi\mathsf{m}!/(\mathsf{m}-i)!=\prod_{q=0}^{i-1}(\mathsf{m}-q)\le\mathsf{m}^{i} (claim 5 of Properties of Finite Products); and for i≥2i\ge2, i!≥2 (i−2)!i!\ge2\,(i-2)!, so with x=m2/μx=\mathsf{m}^{2}/\mu, ∑i=2mxii!≤x22∑i=2mxi−2(i−2)!≤x22exp⁡(x)\sum_{i=2}^{\mathsf{m}}\frac{x^{i}}{i!}\le\frac{x^{2}}{2}\sum_{i=2}^{\mathsf{m}}\frac{x^{i-2}}{(i-2)!}\le\frac{x^{2}}{2}\exp(x) by the series for exp⁡\exp (The Real Exponential Function), all terms being nonnegative. Adding the i=1i=1 term gives the upper bound.

Step 4: claim 4. For k≥mk\ge\mathsf{m}, each factor satisfies 0≤(k−m+i)/μ≤k/μ0\le(k-\mathsf{m}+i)/\mu\le k/\mu, so ϱ(k)≤(k/μ)m\varrho(k)\le(k/\mu)^{\mathsf{m}} by claim 5 of Properties of Finite Products; for k<mk<\mathsf{m}, ϱ(k)=0≤(k/μ)m\varrho(k)=0\le(k/\mu)^{\mathsf{m}}. Now let x≥0x\ge0 with m(x+m)≤μ\mathsf{m}(x+\mathsf{m})\le\mu and let k≥μ−xk\ge\mu-x. Then k≥m(x+m)−x≥m2≥mk\ge\mathsf{m}(x+\mathsf{m})-x\ge\mathsf{m}^{2}\ge\mathsf{m} (as mx≥x\mathsf{m}x\ge x), so every factor satisfies (k−m+i)/μ≥(k−m)/μ≥(μ−x−m)/μ=1−δ(k-\mathsf{m}+i)/\mu\ge(k-\mathsf{m})/\mu\ge(\mu-x-\mathsf{m})/\mu=1-\delta with δ=(x+m)/μ∈[0,1]\delta=(x+\mathsf{m})/\mu\in[0,1] (as m≥1\mathsf{m}\ge1 gives x+m≤m(x+m)≤μx+\mathsf{m}\le\mathsf{m}(x+\mathsf{m})\le\mu), hence ϱ(k)≥(1−δ)m\varrho(k)\ge(1-\delta)^{\mathsf{m}} by claim 5 of Properties of Finite Products. Finally (1−δ)m≥1−mδ(1-\delta)^{m}\ge1-m\delta for every natural number mm and δ∈[0,1]\delta\in[0,1], by induction: it holds for m=1m=1, and multiplying (1−δ)m≥1−mδ(1-\delta)^{m}\ge1-m\delta by 1−δ≥01-\delta\ge0 gives (1−δ)m+1≥(1−mδ)(1−δ)=1−(m+1)δ+mδ2≥1−(m+1)δ(1-\delta)^{m+1}\ge(1-m\delta)(1-\delta)=1-(m+1)\delta+m\delta^{2}\ge1-(m+1)\delta. With m=mm=\mathsf{m} this yields ϱ(k)≥1−m(x+m)/μ\varrho(k)\ge1-\mathsf{m}(x+\mathsf{m})/\mu. ■\blacksquare

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