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Proof of 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

lemmalem:copy-clocks-poisson-increments-2026a
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Reason: Proof of lem:copy-clocks-poisson-increments-2026a: decomposition over the cell-count block, independence of U and V, and the conditional-law claim of the uniform representation.

Proof

Throughout, "measurable" for a real-valued map means measurable with respect to the relevant σ\sigma-algebra and B(R)\mathcal{B}(\mathbb{R}); we use claims 1 to 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions for constants, indicators, sums and products of measurable maps, and claims 2 and 4 of Basic Properties of a Measure (monotonicity, countable subadditivity) together with countable additivity of PP (Measure, Measure Space, and Probability Measure). Generic Borel sets are written BB', the letter BB being the rate bound. Fix a transition label cc for the whole proof, and write z=yc,=(yc,1,,yc,Jc)N0Jcz=y_{c,\cdot}=(y_{c,1},\dots,y_{c,J_c})\in\mathbb{N}_0^{J_c} for the cc-block of a vector yN0Ly\in\mathbb{N}_0^{\mathsf{L}}.

Step 0 (the clocks depend on yy only through the cc-block). By the definition of the deterministic-count clocks in The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record, Pu(y),c=1Ω0Uj=1Jci=1yc,j1{Uic,ju}\mathsf{P}^{(y),c}_u=\mathbf{1}_{\Omega^{U}_0}\sum_{j=1}^{J_c}\sum_{i=1}^{y_{c,j}}\mathbf{1}\{U^{c,j}_i\le u\} involves yy only through yc,y_{c,\cdot}. Hence for zN0Jcz\in\mathbb{N}_0^{J_c} we may write P[z],c\mathsf{P}^{[z],c} for P(y),c\mathsf{P}^{(y),c} with any yy satisfying yc,=zy_{c,\cdot}=z (a notation coined here), and Pu,c(ω)=Pu[Kc,(ω)],c(ω)\mathsf{P}^{\sharp,c}_u(\omega)=\mathsf{P}^{[\mathsf{K}_{c,\cdot}(\omega)],c}_u(\omega) for every ω\omega and u0u\ge0, the cc-block of K(ω)\mathsf{K}(\omega) being Kc,(ω)\mathsf{K}_{c,\cdot}(\omega). By claim 2 of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record, each Pu[z],c\mathsf{P}^{[z],c}_u is U\mathcal{U}-measurable, and Pu[z],c(ω)=puc,(z)(ω)\mathsf{P}^{[z],c}_u(\omega)=p^{c,(z)}_u(\omega) for ωΩ0U\omega\in\Omega^{U}_0 and u[0,R]u\in[0,R]. By claim 1 of the same lemma, Ω0UU\Omega^{U}_0\in\mathcal{U} with P(Ω0U)=1P(\Omega^{U}_0)=1, each Kc,j\mathsf{K}_{c,j} is V\mathcal{V}-measurable with values in N0\mathbb{N}_0, and U\mathcal{U} and V\mathcal{V} are independent, i.e. P(AA)=P(A)P(A)P(A\cap A')=P(A)P(A') for AVA\in\mathcal{V} and AUA'\in\mathcal{U}.

Step 1 (claim 1). Fix rr, 0u0<<urR0\le u_0<\dots<u_r\le R and B1,,BrB'_1,\dots,B'_r as in claim 1. Write EE^{\sharp} for the event on the left of the display in claim 1, and for zN0Jcz\in\mathbb{N}_0^{J_c} put Ez=k=1r{Puk[z],cPuk1[z],cBk},Ez=k=1r{pukc,(z)puk1c,(z)Bk},Dz={Kc,=z}=j=1Jc{Kc,j=zj}.E_z=\bigcap_{k=1}^{r}\bigl\{\mathsf{P}^{[z],c}_{u_k}-\mathsf{P}^{[z],c}_{u_{k-1}}\in B'_k\bigr\},\qquad E'_z=\bigcap_{k=1}^{r}\bigl\{p^{c,(z)}_{u_k}-p^{c,(z)}_{u_{k-1}}\in B'_k\bigr\},\qquad D_z=\{\mathsf{K}_{c,\cdot}=z\}=\bigcap_{j=1}^{J_c}\{\mathsf{K}_{c,j}=z_j\}. Then EzUE_z\in\mathcal{U} (preimages of Borel sets under U\mathcal{U}-measurable differences), DzVD_z\in\mathcal{V}, and EzFE'_z\in\mathcal{F} (each puc,(z)p^{c,(z)}_u is a random variable by claim 2 of Uniform Representation of the Rate-One Poisson Counting Path on a Bounded Interval: Distinct Points, Poisson Increments, Conditional Law Given the Cell Counts, and Point Insertion). The events DzD_z, zN0Jcz\in\mathbb{N}_0^{J_c}, are pairwise disjoint with union Ω\Omega, because Kc,\mathsf{K}_{c,\cdot} takes values in N0Jc\mathbb{N}_0^{J_c}. The set N0Jc\mathbb{N}_0^{J_c} is countable: N0=N{0}\mathbb{N}_0=\mathbb{N}\cup\{0\} is countable by claims 1 and 6 of Basic Properties of Countable Sets, and its JcJ_c-th power is countable by claim 2 of Products and Powers of Countable Sets. Fix a sequence (zn)nN(z_n)_{n\in\mathbb{N}} whose set of terms is N0Jc\mathbb{N}_0^{J_c}. Whenever below we sum a family (P(Az))zN0Jc(P(A_z))_{z\in\mathbb{N}_0^{J_c}} of probabilities of pairwise disjoint events AzA_z, we mean the sum nNP(An)\sum_{n\in\mathbb{N}}P(A'_n) with An=AznA'_n=A_{z_n} if zn{z1,,zn1}z_n\notin\{z_1,\dots,z_{n-1}\} and An=A'_n=\emptyset otherwise; the events AnA'_n are pairwise disjoint with nAn=zAz\bigcup_nA'_n=\bigcup_zA_z, so countable additivity gives P(zAz)=zP(Az)P(\bigcup_zA_z)=\sum_zP(A_z) in this sense, and the same convention (dropping repeated terms) is used for sums of products P(Dz)P(Ez)P(D_z)P(E_z) and P(Dz)P(Ez)P(D_z)P(E'_z), which are then compared term by term.

(a) E=z(DzEz)E^{\sharp}=\bigcup_{z}(D_z\cap E_z). Indeed, for ωDz\omega\in D_z we have Kc,(ω)=z\mathsf{K}_{c,\cdot}(\omega)=z, so by Step 0 Pu,c(ω)=Pu[z],c(ω)\mathsf{P}^{\sharp,c}_u(\omega)=\mathsf{P}^{[z],c}_u(\omega) for every uu, and therefore ωE\omega\in E^{\sharp} if and only if ωEz\omega\in E_z. By countable additivity and the independence of U\mathcal{U} and V\mathcal{V}, P(E)=zP(DzEz)=zP(Dz)P(Ez).P(E^{\sharp})=\sum_{z}P(D_z\cap E_z)=\sum_{z}P(D_z)\,P(E_z).

(b) P(Ez)=P(Ez)P(E_z)=P(E'_z) for every zz. By Step 0, EzΩ0U=EzΩ0UE_z\cap\Omega^{U}_0=E'_z\cap\Omega^{U}_0 (all uku_k lie in [0,R][0,R]), so each of EzE_z, EzE'_z is contained in the union of the other with ΩΩ0U\Omega\setminus\Omega^{U}_0, and monotonicity with subadditivity give P(Ez)P(Ez)+P(ΩΩ0U)=P(Ez)P(E_z)\le P(E'_z)+P(\Omega\setminus\Omega^{U}_0)=P(E'_z) and symmetrically P(Ez)P(Ez)P(E'_z)\le P(E_z), using P(ΩΩ0U)=1P(Ω0U)=0P(\Omega\setminus\Omega^{U}_0)=1-P(\Omega^{U}_0)=0 (claim 3 of Basic Properties of a Measure).

(c) The conditional-law identity. Let R[0,R]\mathbb{R}^{[0,R]} carry the cylinder σ\sigma-algebra C\mathcal{C} of Uniform Representation of the Rate-One Poisson Counting Path on a Bounded Interval: Distinct Points, Poisson Increments, Conditional Law Given the Cell Counts, and Point Insertion, generated by the coordinate maps evu\mathrm{ev}_u, and put F=1A,A=k=1r{xR[0,R]: evuk(x)evuk1(x)Bk}.F=\mathbf{1}_{A},\qquad A=\bigcap_{k=1}^{r}\bigl\{x\in\mathbb{R}^{[0,R]}:\ \mathrm{ev}_{u_k}(x)-\mathrm{ev}_{u_{k-1}}(x)\in B'_k\bigr\}. Each evu\mathrm{ev}_u is measurable from C\mathcal{C} to B(R)\mathcal{B}(\mathbb{R}) (the sets evu1(B)\mathrm{ev}_u^{-1}(B') generate C\mathcal{C}), so each difference evukevuk1\mathrm{ev}_{u_k}-\mathrm{ev}_{u_{k-1}} is measurable, AA is a finite intersection of preimages of Borel sets and lies in C\mathcal{C}, and F:R[0,R][0,]F:\mathbb{R}^{[0,R]}\to[0,\infty] is C\mathcal{C}-measurable. For the maps pc,pc,(z):ΩR[0,R]p^{c},p^{c,(z)}:\Omega\to\mathbb{R}^{[0,R]} (measurable with respect to F\mathcal{F} and C\mathcal{C} by claim 3 of Uniform Representation of the Rate-One Poisson Counting Path on a Bounded Interval: Distinct Points, Poisson Increments, Conditional Law Given the Cell Counts, and Point Insertion) we have F(pc,(z))=1EzF(p^{c,(z)})=\mathbf{1}_{E'_z} and F(pc)=1EF(p^{c})=\mathbf{1}_{E'}, where E=k=1r{pukcpuk1cBk},E'=\bigcap_{k=1}^{r}\bigl\{p^{c}_{u_k}-p^{c}_{u_{k-1}}\in B'_k\bigr\}, the event on the right of the first equality in claim 1. Claim 3 of Uniform Representation of the Rate-One Poisson Counting Path on a Bounded Interval: Distinct Points, Poisson Increments, Conditional Law Given the Cell Counts, and Point Insertion, applied for the label cc (whose data KcK^{c}, (Vic)i(V^{c}_i)_i, (Uic,j)j,i(U^{c,j}_i)_{j,i} and cells Ic,1,,Ic,JcI_{c,1},\dots,I_{c,J_c} are those of that lemma, as recorded in The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record), with this FF and y=zy=z gives, the expectation of the indicator of an event being the probability of that event (Simple Function and Its Integral), P(EDz)=E[F(pc)1{Kc,=z}]=P(Kc,=z)E[F(pc,(z))]=P(Dz)P(Ez).P(E'\cap D_z)=\mathbb{E}\bigl[F(p^{c})\mathbf{1}\{\mathsf{K}_{c,\cdot}=z\}\bigr]=P(\mathsf{K}_{c,\cdot}=z)\,\mathbb{E}\bigl[F(p^{c,(z)})\bigr]=P(D_z)\,P(E'_z).

(d) Assembly. By (a), (b), (c) and countable additivity over the partition (Dz)z(D_z)_z of Ω\Omega, P(E)=zP(Dz)P(Ez)=zP(Dz)P(Ez)=zP(EDz)=P(E),P(E^{\sharp})=\sum_{z}P(D_z)P(E_z)=\sum_{z}P(D_z)P(E'_z)=\sum_{z}P(E'\cap D_z)=P(E'), which is the first equality of claim 1. For the second, claim 2 of Uniform Representation of the Rate-One Poisson Counting Path on a Bounded Interval: Distinct Points, Poisson Increments, Conditional Law Given the Cell Counts, and Point Insertion states that the increments pu1cpu0c,,purcpur1cp^{c}_{u_1}-p^{c}_{u_0},\dots,p^{c}_{u_r}-p^{c}_{u_{r-1}} are independent with pukcpuk1cp^{c}_{u_k}-p^{c}_{u_{k-1}} Poisson with parameter ukuk1u_k-u_{k-1}; by Independence of Events and of Random Variables (with the full index set) and Distribution and Cumulative Distribution Function of a Random Variable, P(E)=k=1rP(pukcpuk1cBk)=k=1rPukuk1(Bk).P(E')=\prod_{k=1}^{r}P\bigl(p^{c}_{u_k}-p^{c}_{u_{k-1}}\in B'_k\bigr)=\prod_{k=1}^{r}P_{u_k-u_{k-1}}(B'_k).

Step 2 (claim 2). Every path of P,c\mathsf{P}^{\sharp,c} is a counting path by claim 2 of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record, and a counting path vanishes at 00 by condition 1 of Counting Path and Its Jump Times; hence P0,c=0\mathsf{P}^{\sharp,c}_0=0 everywhere. Next let 0u<uR0\le u<u'\le R. Claim 1 with r=1r=1, u0=uu_0=u, u1=uu_1=u' gives P(Pu,cPu,cB)=Puu(B)P(\mathsf{P}^{\sharp,c}_{u'}-\mathsf{P}^{\sharp,c}_{u}\in B')=P_{u'-u}(B') for every Borel set BB'; the increment is a random variable (a difference of the F\mathcal{F}-measurable variables of claim 2 of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record), so its distribution is PuuP_{u'-u}, i.e. it is Poisson with parameter uuu'-u. Finally let 0u0<<urR0\le u_0<\dots<u_r\le R and write Xk=Puk,cPuk1,cX_k=\mathsf{P}^{\sharp,c}_{u_k}-\mathsf{P}^{\sharp,c}_{u_{k-1}}. For Borel sets B1,,BrB'_1,\dots,B'_r and a nonempty S{1,,r}S\subseteq\{1,\dots,r\}, apply claim 1 with BkB'_k replaced by R\mathbb{R} for kSk\notin S (so that {XkR}=Ω\{X_k\in\mathbb{R}\}=\Omega and Pukuk1(R)=1P_{u_k-u_{k-1}}(\mathbb{R})=1): P(kS{XkBk})=kSPukuk1(Bk)=kSP(XkBk)P(\bigcap_{k\in S}\{X_k\in B'_k\})=\prod_{k\in S}P_{u_k-u_{k-1}}(B'_k)=\prod_{k\in S}P(X_k\in B'_k), the last step by the single-increment case just proved. This is the independence of X1,,XrX_1,\dots,X_r in the sense of Independence of Events and of Random Variables.

Step 3 (claim 3). Let nRn\le R be a natural number. Every path of P,c\mathsf{P}^{\sharp,c} is a counting path and every Pu,c\mathsf{P}^{\sharp,c}_u is F\mathcal{F}-measurable by claim 2 of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record, so P,c\mathsf{P}^{\sharp,c} is a stochastic process on (Ω,F,P)(\Omega,\mathcal{F},P) with counting paths; and for integers 0i<inR0\le i<i'\le n\le R the increment Pi,cPi,c\mathsf{P}^{\sharp,c}_{i'}-\mathsf{P}^{\sharp,c}_{i} is Poisson with parameter iii'-i by claim 2. These are exactly the hypotheses of Uniform Window Discrepancy Bound for a Counting Process with Poisson Increments on the Integer Grid for this nn and an arbitrary natural number in the role of the window length called mm there (the mm of the present setting is the control dimension and plays no role here).

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