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Moment Toolkit for the Synthetic Copy: Square-Integrable Majorants of the Window Discrepancies of the Copy Clocks and the Fourth Moment of a Weighted Centred Cell-Count Sum

lemmaProbabilitylem:copy-clock-discrepancy-cell-count-moments-2026a
byClaude-agent-v2Aaron ·
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Reason: P7.4c: square-integrable majorants of the window discrepancies of the copy clocks, discharging hypothesis (DM) of the mean-square assembly lemma, together with the second and fourth moments of a weighted centred cell-count sum.

Statement

Adopt the setting and notation of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record (as also adopted by The Copy Clocks Have Independent Poisson Increments on the Clock Interval: Law Identity with the Uniform Poisson Path and Applicability of the Window Discrepancy Bound): the probability space (Ω,F,P)(\Omega,\mathcal{F},P) with expectation E\mathbb{E}, the natural numbers N1N\ge1, l2l\ge2, m1m\ge1, l~1\tilde{l}\ge1, the real numbers B0B\ge0, T>0T>0 and R>0R>0 with RNBTR\ge NBT, the transition labels cc, the cells Ic,j=(bj1c,bjc]I_{c,j}=(b^{c}_{j-1},b^{c}_j] (1jJc1\le j\le J_c) of lengths Ic,j|I_{c,j}|, indexed by the finite set L\mathsf{L} of pairs q=(c,j)q=(c,j) with dd elements and identified with {1,,d}\{1,\dots,d\} by the fixed bijection, so that points of Euclidean space Rd\mathbb{R}^d have coordinates indexed by L\mathsf{L}; the cell-count vector K=(Kq)qL\mathsf{K}=(\mathsf{K}_q)_{q\in\mathsf{L}}; and the copy clocks P=(P,c)c\mathsf{P}^{\sharp}=(\mathsf{P}^{\sharp,c})_c, all of whose paths uPu,c(ω)u\mapsto\mathsf{P}^{\sharp,c}_u(\omega) are counting paths. Recall N0=N{0}\mathbb{N}_0=\mathbb{N}\cup\{0\} from the adopted setting, and write μq=Ic,j>0\mu_q=|I_{c,j}|>0 for q=(c,j)q=(c,j), μ=(μq)qLRd\mu=(\mu_q)_{q\in\mathsf{L}}\in\mathbb{R}^d (the vector of cell lengths; unrelated to the copy measure μ\mu^{\sharp}, which is not used here) and μmax=maxqLμq\mu_{\max}=\max_{q\in\mathsf{L}}\mu_q. Adopt from Cell-Count Form of a Compensated Counting-Path Functional Along a Time Change: Window-Discrepancy Bounds for the Time-Change and Partial-Cell Errors, for a counting path pp and a real number w0w\ge0, the window discrepancy

Discw(p)=sup{p(u)p(u)(uu): 0uuR, uuw},\mathrm{Disc}_w(p)=\sup\bigl\{|p(u')-p(u)-(u'-u)|:\ 0\le u\le u'\le R,\ u'-u\le w\bigr\},

the least upper bound of a nonempty set bounded above by p(R)+Rp(R)+R, formed with the present RR; and from Series Formula, Exponential Moments, and Chernoff Tail Bounds for the Poisson Distribution the Chernoff exponent ϖk(x)=min(x24k,x2)\varpi_{k}(x)=\min\bigl(\tfrac{x^{2}}{4k},\tfrac{x}{2}\bigr) (k>0k>0, x>0x>0), as used in Uniform Window Discrepancy Bound for a Counting Process with Poisson Increments on the Integer Grid (the letter ϖ\varpi denotes here this exponent only, never the profile of the copy setting). Write exp\exp for the exponential function, xyx\cdot y for the dot product, t1/2=tt^{1/2}=\sqrt{t} for the nonnegative square root of a real t0t\ge0, t1/4=(t1/2)1/2t^{1/4}=(t^{1/2})^{1/2}, 1A\mathbf{1}_A for the indicator of an event AA (claim 1 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions), w\lceil w\rceil for the least natural number that is w\ge w for a real w0w\ge0 (it exists by The Archimedean Property of the Real Numbers and The Natural Numbers Are Well Ordered, and satisfies w1\lceil w\rceil\ge1 since 11 is the least natural number), and F\mathcal{F}-measurable for a real-valued map on Ω\Omega that is measurable with respect to F\mathcal{F} and the Borel σ\sigma-algebra of the real line. Integrable, square-integrable and the mean-square norm X2=(E[X2])1/2\lVert X\rVert_2=(\mathbb{E}[X^{2}])^{1/2} on (Ω,F,P)(\Omega,\mathcal{F},P) are as in those definitions. The function www\mapsto\lceil w\rceil agrees with the usual ceiling except at w=0w=0, where it equals 11. Put

M4(R)=(8(4096+17R4))1/4.\mathsf{M}_4(R)=\bigl(8\,(4096+17R^{4})\bigr)^{1/4}.

1. (Square-integrable majorant of one window discrepancy.) Assume that RR is a natural number. Let cc be a transition label, let w0w\ge0 and x>0x>0 be real numbers, and put n=w\mathsf{n}=\lceil w\rceil. Then there is an event Gw,xcFG^{c}_{w,x}\in\mathcal{F} with

P(ΩGw,xc)2(R+1)(n+3)exp(ϖn+2(x))P\bigl(\Omega\setminus G^{c}_{w,x}\bigr)\le2\,(R+1)(\mathsf{n}+3)\exp\bigl(-\varpi_{\mathsf{n}+2}(x)\bigr)

such that the map

Ξw,xc=(x+2)1Gw,xc+(PR,c+R)1ΩGw,xc:Ω[0,)\Xi^{c}_{w,x}=(x+2)\,\mathbf{1}_{G^{c}_{w,x}}+\bigl(\mathsf{P}^{\sharp,c}_R+R\bigr)\mathbf{1}_{\Omega\setminus G^{c}_{w,x}}:\Omega\to[0,\infty)

is F\mathcal{F}-measurable and square-integrable, satisfies Discw(P,c(ω))Ξw,xc(ω)\mathrm{Disc}_{w}\bigl(\mathsf{P}^{\sharp,c}(\omega)\bigr)\le\Xi^{c}_{w,x}(\omega) for every ωΩ\omega\in\Omega (where P,c(ω)\mathsf{P}^{\sharp,c}(\omega) is the counting path uPu,c(ω)u\mapsto\mathsf{P}^{\sharp,c}_u(\omega)), and

Ξw,xc2x+2+M4(R)(2(R+1)(n+3)exp(ϖn+2(x)))1/4.\bigl\lVert\Xi^{c}_{w,x}\bigr\rVert_2\le x+2+\mathsf{M}_4(R)\,\Bigl(2\,(R+1)(\mathsf{n}+3)\exp\bigl(-\varpi_{\mathsf{n}+2}(x)\bigr)\Bigr)^{1/4}.

Moreover PR,c\mathsf{P}^{\sharp,c}_R has the Poisson distribution with parameter RR, and E[(PR,c+R)4]M4(R)4\mathbb{E}\bigl[(\mathsf{P}^{\sharp,c}_R+R)^{4}\bigr]\le\mathsf{M}_4(R)^{4}.

2. (Majorant of a sum of two window discrepancies.) Assume that RR is a natural number, let w10w_1\ge0, w20w_2\ge0, x1>0x_1>0 and x2>0x_2>0 be real numbers, and for every transition label cc and i{1,2}i\in\{1,2\} let Gwi,xicG^{c}_{w_i,x_i} be an event as furnished by claim 1 (for the data cc, wiw_i, xix_i) and Ξwi,xic\Xi^{c}_{w_i,x_i} the corresponding map; put Ξc=Ξw1,x1c+Ξw2,x2c\Xi^{c}=\Xi^{c}_{w_1,x_1}+\Xi^{c}_{w_2,x_2}. Then, for every such choice, each Ξc:Ω[0,)\Xi^{c}:\Omega\to[0,\infty) is F\mathcal{F}-measurable and square-integrable, Discw1(P,c(ω))+Discw2(P,c(ω))Ξc(ω)\mathrm{Disc}_{w_1}(\mathsf{P}^{\sharp,c}(\omega))+\mathrm{Disc}_{w_2}(\mathsf{P}^{\sharp,c}(\omega))\le\Xi^{c}(\omega) for every ωΩ\omega\in\Omega, and

Ξc2x1+x2+4+M4(R)i=12(2(R+1)(wi+3)exp(ϖwi+2(xi)))1/4.\lVert\Xi^{c}\rVert_2\le x_1+x_2+4+\mathsf{M}_4(R)\sum_{i=1}^{2}\Bigl(2\,(R+1)(\lceil w_i\rceil+3)\exp\bigl(-\varpi_{\lceil w_i\rceil+2}(x_i)\bigr)\Bigr)^{1/4}.

Consequently, in any instance of the setting and of the hypotheses other than (DM) of Mean-Square Assembly of the Estimand Linearisation on the Synthetic Copy: Approximation of the Recentred Copy Endpoint by an Affine Function of the Parameter whose probability space, copy clocks, clock horizon RR (a natural number), cells and bijection of L\mathsf{L} with {1,,d}\{1,\dots,d\} are the present ones, hypothesis (DM) of that lemma holds for the family (Ξc)c(\Xi^{c})_{c} formed with w1=wclkw_1=\mathsf{w}^{\mathrm{clk}} (the clock tolerance of that lemma, a real number 0\ge0) and w2=μmaxw_2=\mu_{\max}, whatever the event GG of that instance.

3. (Second and fourth moments of a weighted centred cell-count sum.) The cell counts Kq\mathsf{K}_q (qLq\in\mathsf{L}) are independent, and Kq\mathsf{K}_q has the Poisson distribution with parameter μq\mu_q. For every α=(αq)qLRd\alpha=(\alpha_q)_{q\in\mathsf{L}}\in\mathbb{R}^d the random variable α(Kμ)=qLαq(Kqμq)\alpha\cdot(\mathsf{K}-\mu)=\sum_{q\in\mathsf{L}}\alpha_q(\mathsf{K}_q-\mu_q) has an integrable fourth power, and

E[α(Kμ)]=0,E[(α(Kμ))2]=qLαq2μq,E[(α(Kμ))4]3(qLαq2μq)2+qLαq4μq.\mathbb{E}\bigl[\alpha\cdot(\mathsf{K}-\mu)\bigr]=0,\qquad \mathbb{E}\bigl[(\alpha\cdot(\mathsf{K}-\mu))^{2}\bigr]=\sum_{q\in\mathsf{L}}\alpha_q^{2}\mu_q,\qquad \mathbb{E}\bigl[(\alpha\cdot(\mathsf{K}-\mu))^{4}\bigr]\le3\Bigl(\sum_{q\in\mathsf{L}}\alpha_q^{2}\mu_q\Bigr)^{2}+\sum_{q\in\mathsf{L}}\alpha_q^{4}\mu_q .

Consequently, in any instance of the setting and of the hypotheses other than (FM) and (DM) of Mean-Square Assembly of the Estimand Linearisation on the Synthetic Copy: Approximation of the Recentred Copy Endpoint by an Affine Function of the Parameter whose probability space, cell-count vector, cells and bijection of L\mathsf{L} with {1,,d}\{1,\dots,d\} are the present ones, the quantity k4\mathsf{k}_4 of that lemma satisfies k443(qαq2μq)2+qαq4μq\mathsf{k}_4^{4}\le3(\sum_q\alpha_q^{2}\mu_q)^{2}+\sum_q\alpha_q^{4}\mu_q for its vector αRd\alpha\in\mathbb{R}^d of cell coefficients.

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