TheoremBase

Proof

Throughout, a composition g∘fg\circ f of measurable maps is measurable, since (g∘f)−1(E)=f−1(g−1(E))(g\circ f)^{-1}(E)=f^{-1}(g^{-1}(E)); a map into a product of two measurable spaces whose two coordinates are measurable is measurable with respect to the product σ\sigma-algebra, by claim 2 of Generator Criterion for Measurability applied to the generating rectangles, whose preimages are intersections of the two coordinate preimages (the rectangle argument); and for x∈Δlx\in\Delta^{l} one has ∣x∣≤1|x|\le1, because xγ≥0x^{\gamma}\ge0, ∑γxγ=1\sum_{\gamma}x^{\gamma}=1 and ∣x∣2=∑γ(xγ)2≤(∑γxγ)2=1|x|^{2}=\sum_{\gamma}(x^{\gamma})^{2}\le(\sum_{\gamma}x^{\gamma})^{2}=1 (claim 1 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square, the cross terms being nonnegative), so that ∣x−y∣≤2|x-y|\le2 for x,y∈Δlx,y\in\Delta^{l} by claims 5 and 6 there (this is also recorded in claim 4 of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy). Monotonicity, positive homogeneity and additivity of integrals of nonnegative measurable functions are those of Linearity and Monotonicity of the Lebesgue Integral, and ∫1A dν=ν(A)\int\mathbf{1}_{A}\,d\nu=\nu(A) is The Integral of an Indicator Function is the Measure of the Set. We use repeatedly that for real numbers 0≤a≤b0\le a\le b one has a2≤b2a^{2}\le b^{2}, a4≤b4a^{4}\le b^{4}, a1/2≤b1/2a^{1/2}\le b^{1/2} and a1/4≤b1/4a^{1/4}\le b^{1/4}, by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field applied once or twice in either direction.

Claim 1. (a) The setting of Law Identity between the N-Agent Aggregate Path with Its Observation Record and the Synthetic Copy's Regularised Path with Its Record with horizon ss requires the setting of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record with the horizon ss (adopted on the copy side, with its probability space (Ω,F,P)(\Omega,\mathcal{F},P) in the role of (Ω♭,F♭,P♭)(\Omega^{\flat},\mathcal{F}^{\flat},P^{\flat}) and x0\mathsf{x}_{0} in the role of x0x_{0}), the strict inequality R>NBsR>NBs (hypothesis (L)), an NN-agent driving system with ll states and l~\tilde{l} channels (here (Ωag,Fag,Pag)(\Omega^{\mathrm{ag}},\mathcal{F}^{\mathrm{ag}},P^{\mathrm{ag}})), a solution of the controlled NN-agent dynamics on [0,s][0,s] for the policy of the copy side and for the same data mm, A\mathcal{A}, β\beta, BB, β~\tilde{\beta}, B~\tilde{B} and horizon (here the restricted solution, which is a solution on [0,s][0,s] for h(s)h^{(s)} on this driving system by the setting of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy, the data being the same by (L)), and reconstruction data for this driving system and h(s)h^{(s)} with horizon ss (fixed in the adopted setting). Thus that setting is instantiated. The additional hypotheses of claim 5 of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy are exactly this instantiation together with Pag(Σ0=x0)=1P^{\mathrm{ag}}(\Sigma_{0}=\mathsf{x}_{0})=1, which is part of (L); hence its claims 1--5 are available. For r∈Rsr\in\mathbf{R}_{s} and t∈[0,s]t\in[0,s], the record-frozen flow of (AF) is Φtr=St(s)(z0,ar)\Phi^{r}_{t}=\mathsf{S}^{(s)}_{t}(z_{0},a^{r}), the mean-field flow with horizon ss of claim 2 of Stability of the Mean-Field Flow under Perturbation of the Initial State and Weak Convergence of Controls evaluated at the base point and at the class of the record-frozen control path of the copy side's policy at rr; by (L) the base point is S0S_{0} and that path is a(s),ra^{(s),r}, so Φtr=St(s)(S0,a(s),r)=Φt(s),r\Phi^{r}_{t}=\mathsf{S}^{(s)}_{t}(S_{0},a^{(s),r})=\Phi^{(s),r}_{t} (the dense sequence entering neither flow). Consequently X′′(ω,r)=N(Σˉs♯,r(ω)−Φsr)=N(Σˉs♯,r(ω)−Φs(s),r)=Xs′′(ω,θ,r)X''(\omega,r)=\sqrt{N}(\bar\Sigma^{\sharp,r}_{s}(\omega)-\Phi^{r}_{s})=\sqrt{N}(\bar\Sigma^{\sharp,r}_{s}(\omega)-\Phi^{(s),r}_{s})=X''_{s}(\omega,\theta,r) for every (ω,θ,r)∈Ω♯(\omega,\theta,r)\in\Omega^{\sharp}, by the defining formulas.

(b) By claim 1 of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy, the Data paragraph of The Realized Control as the Record-Frozen Control at the Observation Record, and Measurability of the Path-and-Record Closeness Set is instantiated with horizon ss by the NN-agent data, the policy h(s)h^{(s)}, the restricted solution and the fixed dense sequence. For the comparison data: each component of t↦Stt\mapsto S_{t} is continuous on [0,T][0,T], hence its restriction to [0,s][0,s] is continuous on [0,s][0,s] (given t0∈[0,s]t_{0}\in[0,s] and ε>0\varepsilon>0, a δ>0\delta>0 serving for all t∈[0,T]t\in[0,T] with ∣t−t0∣<δ|t-t_{0}|<\delta serves in particular for all such t∈[0,s]t\in[0,s], which is continuity relative to [0,s][0,s]); ∣St∣≤1=K∗|S_{t}|\le1=K^{*} because St∈ΔlS_{t}\in\Delta^{l}; and t↦Att\mapsto A_{t} (t∈[0,s]t\in[0,s]) takes values in A\mathcal{A} with components continuous on [0,s][0,s] (by the same restriction argument), hence measurable with respect to B[0,s]\mathcal{B}_{[0,s]} by claim 4 of Measurability of Countable Suprema, Bounded Pointwise Limits, Monotone Functions, and Continuous Functions. For the path data: GN\mathbb{G}_{N} is a nonempty finite subset of Rl\mathbb{R}^{l}, since it contains Σ0(ω)\Sigma_{0}(\omega) for any ω\omega (claim 4 of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy) and, by its definition in Open-Loop Aggregate Solution Driven by Aggregate Transition Clocks (NxγNx^{\gamma} a nonnegative integer for every γ\gamma, and 0≤xγ≤10\le x^{\gamma}\le1 on Δl\Delta^{l}), is contained in the finite set of points xx with Nxγ∈{0,1,…,N}Nx^{\gamma}\in\{0,1,\dots,N\} for all γ\gamma. Thus the whole setting of The Realized Control as the Record-Frozen Control at the Observation Record, and Measurability of the Path-and-Record Closeness Set is instantiated with horizon ss, and its claims 2, 3 and 4 furnish d\mathsf{d}, s\mathsf{s} and E(ε,ε′)∈C⊗Rs\mathsf{E}(\varepsilon,\varepsilon')\in\mathcal{C}\otimes\mathcal{R}_{s} (the σ\sigma-algebra written Cs\mathcal{C}_{s} there being C\mathcal{C}, both generated by the sets {p:p(t)=y}\{p:p(t)=y\}), with s(p)=sup⁡t∈[0,s]∣p(t)−St∣\mathsf{s}(p)=\sup_{t\in[0,s]}|p(t)-S_{t}| and d(r)=∫[0,s]∣a(s),r(t)−At∣ dt\mathsf{d}(r)=\int_{[0,s]}|a^{(s),r}(t)-A_{t}|\,dt as displayed. Finally, for ω∈Ω0ag\omega\in\Omega^{\mathrm{ag}}_{0}, claim 2 of that lemma applied to the restricted solution, whose record is W(s)W^{(s)} and whose realized control is α^(s)\hat{\alpha}^{(s)}, gives d(W(s)(ω))=∫[0,s]∣α^(s)(t,ω)−At∣ dt\mathsf{d}(W^{(s)}(\omega))=\int_{[0,s]}|\hat{\alpha}^{(s)}(t,\omega)-A_{t}|\,dt, and α^(s)(t,ω)=α^(t,ω)\hat{\alpha}^{(s)}(t,\omega)=\hat{\alpha}(t,\omega) for t∈[0,s]t\in[0,s] by claim 3 of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy.

Claim 2. Fix r∈Rsr\in\mathbf{R}_{s}, t∈[0,s]t\in[0,s] and a label c=(σ,γ0)∈Lc=(\sigma,\gamma_{0})\in\mathcal{L}, and write a=a(s),r(t)a=a^{(s),r}(t) and a′=Ata'=A_{t}; both lie in A\mathcal{A} (claim 1 of The Record-Frozen Control as a Measurable Map into the Weakly Metrized Control Set, and the Record-Frozen Mean-Field Flow: Joint Measurability, Flow Equation, and Measurability in the Record with horizon ss, available by claim 1 of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy; and AA takes its values in A\mathcal{A} because (S,A)(S,A) is a mean-field trajectory pair for β\beta, as recorded in the adopted NN-agent setting), and St∈ΔlS_{t}\in\Delta^{l}. Let (U,Wβ,βˉ)(U,W_{\beta},\bar\beta) be the twice continuously differentiable extension of (X), with Δl⊂U\Delta^{l}\subset U and A⊆Wβ\mathcal{A}\subseteq W_{\beta}, both open and convex, so that U×WβU\times W_{\beta} is an open subset of Rl+m\mathbb{R}^{l+m} (condition 2 of that definition). The segment {(St,a+τ(a′−a)):τ∈[0,1]}\{(S_{t},a+\tau(a'-a)):\tau\in[0,1]\} between the points x=(St,a)x=(S_{t},a) and y=(St,a′)y=(S_{t},a') of Rl+m\mathbb{R}^{l+m} lies in Δl×A⊆U×Wβ\Delta^{l}\times\mathcal{A}\subseteq U\times W_{\beta}, because A\mathcal{A} is convex; and ∣y−x∣=∣a′−a∣|y-x|=|a'-a|, the first ll coordinates of y−xy-x vanishing (claim 1 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square). By claim 1 of Shared-Clock Point Insertion into the Open-Loop Aggregate Solution: Exact Response Identity, Crude Bound, and Linearisation Defect (in the instance of its setting fixed by the adopted copy setting through Closeness to a Mean-Field Pair on the Synthetic Copy: Clock Discrepancy, Gronwall Comparison of the Weighted Response with the Profile Response, and the Observation-Information Bound with Mean-Field Data), ψc\psi_{c} is of class C2C^{2} on U×WβU\times W_{\beta}, hence of class C1C^{1} there (clause 2 of C^k Maps on a Euclidean Open Set), and at every point of Δl×A\Delta^{l}\times\mathcal{A}, in particular at every point of the segment, ∣∂iψc∣≤B+K|\partial_{i}\psi_{c}|\le B+K and ∣∂j∂iψc∣≤3K|\partial_{j}\partial_{i}\psi_{c}|\le3K for all i,j∈{1,…,l+m}i,j\in\{1,\dots,l+m\}. Part (i) of Multivariate Taylor Expansion with Uniform Second-Order Remainder, applied with n=l+mn=l+m, W=U×WβW=U\times W_{\beta}, f=ψcf=\psi_{c} and M1=B+KM_{1}=B+K, gives

∣ψc(St,a′)−ψc(St,a)∣≤l+m (B+K) ∣a′−a∣=Λ1∣a′−a∣.|\psi_{c}(S_{t},a')-\psi_{c}(S_{t},a)|\le\sqrt{l+m}\,(B+K)\,|a'-a|=\Lambda_{1}|a'-a| .

For γ∈{1,…,l}\gamma\in\{1,\dots,l\} the function ∂γψc\partial_{\gamma}\psi_{c} is of class C1C^{1} on U×WβU\times W_{\beta} (clause 2 of C^k Maps on a Euclidean Open Set, ψc\psi_{c} being of class C2C^{2}), and its partial derivatives ∂j∂γψc\partial_{j}\partial_{\gamma}\psi_{c} are bounded by 3K3K on the segment; part (i) of the Taylor lemma with f=∂γψcf=\partial_{\gamma}\psi_{c} and M1=3KM_{1}=3K gives ∣∂γψc(St,a′)−∂γψc(St,a)∣≤l+m 3K ∣a′−a∣|\partial_{\gamma}\psi_{c}(S_{t},a')-\partial_{\gamma}\psi_{c}(S_{t},a)|\le\sqrt{l+m}\,3K\,|a'-a|. Since gc=(∂1ψc,…,∂lψc)g^{c}=(\partial_{1}\psi_{c},\dots,\partial_{l}\psi_{c}), the vector gc(St,a′)−gc(St,a)g^{c}(S_{t},a')-g^{c}(S_{t},a) has ll components each of absolute value at most l+m 3K∣a′−a∣\sqrt{l+m}\,3K|a'-a|, so its squared norm is at most l (l+m) 9K2∣a′−a∣2l\,(l+m)\,9K^{2}|a'-a|^{2} (claim 1 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square) and

∣gc(St,a′)−gc(St,a)∣≤ll+m 3K ∣a′−a∣=Λ3∣a′−a∣.|g^{c}(S_{t},a')-g^{c}(S_{t},a)|\le\sqrt{l}\sqrt{l+m}\,3K\,|a'-a|=\Lambda_{3}|a'-a| .

Summing the two bounds over the l(l−1)l(l-1) labels gives the displayed inequality of claim 2 with CLip=l(l−1)(Λ1+Λ3)C_{\mathrm{Lip}}=l(l-1)(\Lambda_{1}+\Lambda_{3}). The integrand of Dctlr\mathsf{D}^{r}_{\mathrm{ctl}} (the left-hand side as a function of tt, with the comparison pair (S,A)(S,A) on [0,s][0,s] by (L)) is bounded and measurable by claim 1 of Closeness to a Mean-Field Pair on the Synthetic Copy: Clock Discrepancy, Gronwall Comparison of the Weighted Response with the Profile Response, and the Observation-Information Bound with Mean-Field Data, and t↦∣a(s),r(t)−At∣t\mapsto|a^{(s),r}(t)-A_{t}| is measurable by claim 2 of The Realized Control as the Record-Frozen Control at the Observation Record, and Measurability of the Path-and-Record Closeness Set; integrating the pointwise inequality over [0,s][0,s] (monotonicity and positive homogeneity) gives Dctlr≤CLip∫[0,s]∣a(s),r(t)−At∣ dt=CLip d(r)\mathsf{D}^{r}_{\mathrm{ctl}}\le C_{\mathrm{Lip}}\int_{[0,s]}|a^{(s),r}(t)-A_{t}|\,dt=C_{\mathrm{Lip}}\,\mathsf{d}(r).

Claim 3. The tolerances. Both tolerances are nonnegative real numbers: εS(N)=(Cflw+1)N−1/4\varepsilon_{S}(N)=(C_{\mathrm{flw}}+1)N^{-1/4} and εctl(N)=(TCctl)1/2N−1/4\varepsilon_{\mathrm{ctl}}(N)=(TC_{\mathrm{ctl}})^{1/2}N^{-1/4} are nonnegative, because N−1/4>0N^{-1/4}>0, Cctl=2(Z♯+1)>0C_{\mathrm{ctl}}=2(\mathcal{Z}^{\sharp}+1)>0 with Z♯≥0\mathcal{Z}^{\sharp}\ge0 (claims 3 and 4 of Closeness of the Realized Control and the Realized Mean-Field Flow on a High-Probability Event under the Cost Bound), (TCctl)1/2(TC_{\mathrm{ctl}})^{1/2} is a nonnegative square root, and Cflw=CSCctl1/2C_{\mathrm{flw}}=C_{S}C_{\mathrm{ctl}}^{1/2} with CS=eΛbTl K2TC_{S}=e^{\Lambda_{b}T}\sqrt{l}\,K_{2}\sqrt{T} (claim 4 there) is nonnegative, K2=2l(l−1)K1K_{2}=2\sqrt{l}(l-1)K_{1} being nonnegative since K1≥0K_{1}\ge0 by claim 1 of The Transition-Rate Family and Aggregate Drift of Affine-Controlled Data; and CLip=l(l−1)(Λ1+Λ3)≥0C_{\mathrm{Lip}}=l(l-1)(\Lambda_{1}+\Lambda_{3})\ge0 since B,K≥0B,K\ge0. This is the first clause of (CL), so that, from here on, (CP) holds in full with wclk=N(Λ1s εS+εctl)≥0\mathsf{w}^{\mathrm{clk}}=N(\Lambda_{1}s\,\varepsilon_{S}+\varepsilon_{\mathrm{ctl}})\ge0, and claims 1 and 2 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 are available by its scope statement.

Joint measurability of the regularised paths. Write Πˉ(ω,r)=Σˉ♯,r(ω)∈Path\bar\Pi(\omega,r)=\bar\Sigma^{\sharp,r}(\omega)\in\mathsf{Path} for (ω,r)∈Ω×Rs(\omega,r)\in\Omega\times\mathbf{R}_{s}; this is Π♯(ω,0,r)\Pi^{\sharp}(\omega,0,r) for the map Π♯\Pi^{\sharp} of Law Identity between the N-Agent Aggregate Path with Its Observation Record and the Synthetic Copy's Regularised Path with Its Record, which takes its values in Path\mathsf{Path} and is measurable with respect to (F⊗B(Rd))⊗Rs(\mathcal{F}\otimes\mathcal{B}(\mathbb{R}^{d}))\otimes\mathcal{R}_{s} and C\mathcal{C} by its claim 1 (available by claim 1(a)). By claim 4 of Sections of Product-Measurable Sets and Maps Are Measurable, and Insertion Maps into Products Are Measurable (fixing the middle coordinate 0∈Rd0\in\mathbb{R}^{d}), Πˉ\bar\Pi is measurable with respect to F⊗Rs\mathcal{F}\otimes\mathcal{R}_{s} and C\mathcal{C}. By the rectangle argument the map (ω,r)↦(Πˉ(ω,r),r)(\omega,r)\mapsto(\bar\Pi(\omega,r),r) is measurable with respect to F⊗Rs\mathcal{F}\otimes\mathcal{R}_{s} and C⊗Rs\mathcal{C}\otimes\mathcal{R}_{s} (its second coordinate being the projection, measurable by claim 5 of Sections of Product-Measurable Sets and Maps Are Measurable, and Insertion Maps into Products Are Measurable), so, writing E=E(εS(N),εctl(N))∈C⊗Rs\mathsf{E}=\mathsf{E}(\varepsilon_{S}(N),\varepsilon_{\mathrm{ctl}}(N))\in\mathcal{C}\otimes\mathcal{R}_{s} (claim 1(b)), the set

B={(ω,r)∈Ω×Rs: (Πˉ(ω,r),r)∉E}\mathsf{B}=\bigl\{(\omega,r)\in\Omega\times\mathbf{R}_{s}:\ (\bar\Pi(\omega,r),r)\notin\mathsf{E}\bigr\}

belongs to F⊗Rs\mathcal{F}\otimes\mathcal{R}_{s}, and its sections Bω={r:(ω,r)∈B}\mathsf{B}_{\omega}=\{r:(\omega,r)\in\mathsf{B}\} belong to Rs\mathcal{R}_{s} for every ω\omega (claim 1 of Sections of Product-Measurable Sets and Maps Are Measurable, and Insertion Maps into Products Are Measurable). For ω∈G∩Ω′\omega\in G\cap\Omega' one has Rωcl=Tω∩(Rs∖Bω)\mathsf{R}^{\mathrm{cl}}_{\omega}=\mathsf{T}_{\omega}\cap(\mathbf{R}_{s}\setminus\mathsf{B}_{\omega}).

Membership and inclusion. For ω∉G∩Ω′\omega\notin G\cap\Omega', Rωcl=∅∈Rs\mathsf{R}^{\mathrm{cl}}_{\omega}=\emptyset\in\mathcal{R}_{s} and ∅⊆Tω\emptyset\subseteq\mathsf{T}_{\omega}. For ω∈G∩Ω′\omega\in G\cap\Omega', Rs∖Tω∈Rs\mathbf{R}_{s}\setminus\mathsf{T}_{\omega}\in\mathcal{R}_{s} by claim 3 of Almost Sure Tracking on the Synthetic Copy: Jump Times of the Deterministic-Count Clocks, Almost Sure Conflict-Freeness of Every Record, Almost Sure Null Mass of the Untracked Records, and Trimming an Event to the Tracked Set (its setting being that of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record with the move size m\mathsf{m}, adopted), so Tω∈Rs\mathsf{T}_{\omega}\in\mathcal{R}_{s}, hence Rωcl∈Rs\mathsf{R}^{\mathrm{cl}}_{\omega}\in\mathcal{R}_{s} as an intersection of two members, and Rωcl⊆Tω\mathsf{R}^{\mathrm{cl}}_{\omega}\subseteq\mathsf{T}_{\omega} by construction.

Closeness on the close records. Let ω∈G\omega\in G and r∈Rωclr\in\mathsf{R}^{\mathrm{cl}}_{\omega}; then ω∈G∩Ω′\omega\in G\cap\Omega' (otherwise Rωcl\mathsf{R}^{\mathrm{cl}}_{\omega} is empty) and (Σˉ♯,r(ω),r)∈E(\bar\Sigma^{\sharp,r}(\omega),r)\in\mathsf{E}, that is, s(Σˉ♯,r(ω))≤εS(N)\mathsf{s}(\bar\Sigma^{\sharp,r}(\omega))\le\varepsilon_{S}(N) and d(r)≤εctl(N)\mathsf{d}(r)\le\varepsilon_{\mathrm{ctl}}(N). The first gives ∣Σˉt♯,r(ω)−St∣≤s(Σˉ♯,r(ω))≤εS(N)=εS|\bar\Sigma^{\sharp,r}_{t}(\omega)-S_{t}|\le\mathsf{s}(\bar\Sigma^{\sharp,r}(\omega))\le\varepsilon_{S}(N)=\varepsilon_{S} for every t∈[0,s]t\in[0,s], the path deviation being the least upper bound of these distances; the second gives, by claim 2, Dctlr≤CLip d(r)≤CLip εctl(N)=εctl\mathsf{D}^{r}_{\mathrm{ctl}}\le C_{\mathrm{Lip}}\,\mathsf{d}(r)\le C_{\mathrm{Lip}}\,\varepsilon_{\mathrm{ctl}}(N)=\varepsilon_{\mathrm{ctl}}.

Integrals over ρ\rho-null sets vanish. Let ω∈Ω\omega\in\Omega and let N∈Rs\mathsf{N}\in\mathcal{R}_{s} with ρ(N)=0\rho(\mathsf{N})=0. The map r↦ℓ♯,ω(r)r\mapsto\ell^{\sharp,\omega}(r) is Rs\mathcal{R}_{s}-measurable with values in [0,∞)[0,\infty) (a section of the Rs⊗F\mathcal{R}_{s}\otimes\mathcal{F}-measurable map of claim 3 of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record, by claim 3 of Sections of Product-Measurable Sets and Maps Are Measurable, and Insertion Maps into Products Are Measurable). For natural numbers nn put fn=min⁡(ℓ♯,ω,n) 1Nf_{n}=\min(\ell^{\sharp,\omega},n)\,\mathbf{1}_{\mathsf{N}}, measurable by claims 1, 3 and 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, nonnegative, with fn≤fn+1f_{n}\le f_{n+1} and sup⁡nfn=ℓ♯,ω1N\sup_{n}f_{n}=\ell^{\sharp,\omega}\mathbf{1}_{\mathsf{N}} pointwise (the value ℓ♯,ω(r)\ell^{\sharp,\omega}(r) being a real number, exceeded by no nn larger than it). Since fn≤n1Nf_{n}\le n\mathbf{1}_{\mathsf{N}}, monotonicity and positive homogeneity give ∫fn dρ≤nρ(N)=0\int f_{n}\,d\rho\le n\rho(\mathsf{N})=0, and Monotone Convergence Theorem gives ∫Rsℓ♯,ω1N dρ=sup⁡n∫fn dρ=0\int_{\mathbf{R}_{s}}\ell^{\sharp,\omega}\mathbf{1}_{\mathsf{N}}\,d\rho=\sup_{n}\int f_{n}\,d\rho=0.

The non-close mass. Since ℓ♯,ω≥0\ell^{\sharp,\omega}\ge0 integrates to 11 against ρ\rho for every ω\omega (claim 3 of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record) and 0≤ℓ♯,ω1Rs∖Rωcl≤ℓ♯,ω0\le\ell^{\sharp,\omega}\mathbf{1}_{\mathbf{R}_{s}\setminus\mathsf{R}^{\mathrm{cl}}_{\omega}}\le\ell^{\sharp,\omega}, the integral πωnc\pi^{\mathrm{nc}}_{\omega} is defined (the indicator of Rs∖Rωcl∈Rs\mathbf{R}_{s}\setminus\mathsf{R}^{\mathrm{cl}}_{\omega}\in\mathcal{R}_{s} being measurable) and lies in [0,1][0,1] by monotonicity. For ω∉G∩Ω′\omega\notin G\cap\Omega', πωnc=∫ℓ♯,ω dρ=1\pi^{\mathrm{nc}}_{\omega}=\int\ell^{\sharp,\omega}\,d\rho=1. For ω∈G∩Ω′\omega\in G\cap\Omega', the complement of Rωcl=Tω∩(Rs∖Bω)\mathsf{R}^{\mathrm{cl}}_{\omega}=\mathsf{T}_{\omega}\cap(\mathbf{R}_{s}\setminus\mathsf{B}_{\omega}) is the disjoint union of Bω\mathsf{B}_{\omega} and (Rs∖Tω)∖Bω(\mathbf{R}_{s}\setminus\mathsf{T}_{\omega})\setminus\mathsf{B}_{\omega}, so by additivity

πωnc=∫Rsℓ♯,ω1Bω dρ+∫Rsℓ♯,ω1(Rs∖Tω)∖Bω dρ=I(ω),I(ω)=∫Rsℓ♯,ω(r) 1B(ω,r) ρ(dr),\pi^{\mathrm{nc}}_{\omega}=\int_{\mathbf{R}_{s}}\ell^{\sharp,\omega}\mathbf{1}_{\mathsf{B}_{\omega}}\,d\rho+\int_{\mathbf{R}_{s}}\ell^{\sharp,\omega}\mathbf{1}_{(\mathbf{R}_{s}\setminus\mathsf{T}_{\omega})\setminus\mathsf{B}_{\omega}}\,d\rho=I(\omega),\qquad I(\omega)=\int_{\mathbf{R}_{s}}\ell^{\sharp,\omega}(r)\,\mathbf{1}_{\mathsf{B}}(\omega,r)\,\rho(dr),

the second integral vanishing by the previous paragraph, because (Rs∖Tω)∖Bω(\mathbf{R}_{s}\setminus\mathsf{T}_{\omega})\setminus\mathsf{B}_{\omega} is a member of Rs\mathcal{R}_{s} contained in Rs∖Tω\mathbf{R}_{s}\setminus\mathsf{T}_{\omega}, which for ω∈Ω′\omega\in\Omega' belongs to Rs\mathcal{R}_{s} and has ρ\rho-measure 00 by claim 3 of Almost Sure Tracking on the Synthetic Copy: Jump Times of the Deterministic-Count Clocks, Almost Sure Conflict-Freeness of Every Record, Almost Sure Null Mass of the Untracked Records, and Trimming an Event to the Tracked Set, so that the smaller set has ρ\rho-measure 00 by monotonicity of the measure ρ\rho. Now 1B\mathbf{1}_{\mathsf{B}} is an F⊗Rs\mathcal{F}\otimes\mathcal{R}_{s}-measurable map Ω×Rs→[0,∞)\Omega\times\mathbf{R}_{s}\to[0,\infty), so by claim 2 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 (which, by the scope statement preceding its claim 1, holds in the present instance although (CL), (FM) and (DM) have not yet been established) the map ω↦I(ω)\omega\mapsto I(\omega) is F\mathcal{F}-measurable and

E[I]=∫Ω♯1B dμ♯,\mathbb{E}[I]=\int_{\Omega^{\sharp}}\mathbf{1}_{\mathsf{B}}\,d\mu^{\sharp},

1B\mathbf{1}_{\mathsf{B}} being regarded as a function on Ω♯\Omega^{\sharp} through the coordinate maps. Hence πnc=1Ω∖(G∩Ω′)+1G∩Ω′ I\pi^{\mathrm{nc}}=\mathbf{1}_{\Omega\setminus(G\cap\Omega')}+\mathbf{1}_{G\cap\Omega'}\,I is F\mathcal{F}-measurable (claims 1, 2 and 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions; G∈FG\in\mathcal{F} by (G), and Ω′∈F\Omega'\in\mathcal{F} because claim 3 of Almost Sure Tracking on the Synthetic Copy: Jump Times of the Deterministic-Count Clocks, Almost Sure Conflict-Freeness of Every Record, Almost Sure Null Mass of the Untracked Records, and Trimming an Event to the Tracked Set places it in the σ\sigma-algebra generated by the driving variables Uic,jU^{c,j}_{i}, which is contained in F\mathcal{F}). This establishes (CL).

The bound on πˉnc\bar\pi^{\mathrm{nc}}. Pointwise, 1Gπnc=1G∖Ω′+1G∩Ω′I≤1Ω∖Ω′+I\mathbf{1}_{G}\pi^{\mathrm{nc}}=\mathbf{1}_{G\setminus\Omega'}+\mathbf{1}_{G\cap\Omega'}I\le\mathbf{1}_{\Omega\setminus\Omega'}+I, and E[1Ω∖Ω′]=P(Ω∖Ω′)=0\mathbb{E}[\mathbf{1}_{\Omega\setminus\Omega'}]=P(\Omega\setminus\Omega')=0 since P(Ω′)=1P(\Omega')=1 (claim 3 of Almost Sure Tracking on the Synthetic Copy: Jump Times of the Deterministic-Count Clocks, Almost Sure Conflict-Freeness of Every Record, Almost Sure Null Mass of the Untracked Records, and Trimming an Event to the Tracked Set); by monotonicity and additivity, πˉnc≤E[I]\bar\pi^{\mathrm{nc}}\le\mathbb{E}[I]. On Ω♯\Omega^{\sharp}, 1B(ω,r)=1{(Π♯,D)∉E}(ω,θ,r)=F′(Π♯,D)(ω,θ,r)\mathbf{1}_{\mathsf{B}}(\omega,r)=\mathbf{1}\{(\Pi^{\sharp},\mathsf{D})\notin\mathsf{E}\}(\omega,\theta,r)=F'(\Pi^{\sharp},\mathsf{D})(\omega,\theta,r) with F′=1(Path×Rs)∖EF'=\mathbf{1}_{(\mathsf{Path}\times\mathbf{R}_{s})\setminus\mathsf{E}}, a C⊗Rs\mathcal{C}\otimes\mathcal{R}_{s}-measurable map into [0,∞][0,\infty] (claim 1 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions), because Π♯(ω,θ,r)=Πˉ(ω,r)\Pi^{\sharp}(\omega,\theta,r)=\bar\Pi(\omega,r) and D(ω,θ,r)=r\mathsf{D}(\omega,\theta,r)=r. Claim 2 of Law Identity between the N-Agent Aggregate Path with Its Observation Record and the Synthetic Copy's Regularised Path with Its Record with Pag(D0)=1P^{\mathrm{ag}}(D_{0})=1, where D0={Σ0=x0}D_{0}=\{\Sigma_{0}=\mathsf{x}_{0}\}, gives

E[I]=∫Ω♯F′(Π♯,D) dμ♯=Eag[1D0F′(Π,W(s))]≤Eag[F′(Π,W(s))]=Pag({(Π,W(s))∉E}),\mathbb{E}[I]=\int_{\Omega^{\sharp}}F'(\Pi^{\sharp},\mathsf{D})\,d\mu^{\sharp}=\mathbb{E}^{\mathrm{ag}}\bigl[\mathbf{1}_{D_{0}}F'(\Pi,W^{(s)})\bigr]\le\mathbb{E}^{\mathrm{ag}}\bigl[F'(\Pi,W^{(s)})\bigr]=P^{\mathrm{ag}}\bigl(\{(\Pi,W^{(s)})\notin\mathsf{E}\}\bigr),

the record of the restricted solution being W(s)W^{(s)}, and the set {(Π,W(s))∉E}\{(\Pi,W^{(s)})\notin\mathsf{E}\} belonging to Fag\mathcal{F}^{\mathrm{ag}} because Π\Pi and W(s)W^{(s)} are measurable (claim 1 of that lemma) and the pair is measurable by the rectangle argument. Let ω∈ΩNcl\omega\in\Omega^{\mathrm{cl}}_{N}. Then ω∈Ω0ag\omega\in\Omega^{\mathrm{ag}}_{0} by the definition of ΩNcl\Omega^{\mathrm{cl}}_{N} in claim 2 of The Path-Closeness Event under the Cost Bound: Closeness of the Empirical State Measure to the Mean-Field Trajectory and of the Record-Frozen Control to the Mean-Field Control on an Event of Probability 1−O(N−1/2)1-O(N^{-1/2}), so Π(ω)\Pi(\omega) is the path t↦Σt(ω)t\mapsto\Sigma_{t}(\omega) on [0,s][0,s] (definition of Π\Pi in Law Identity between the N-Agent Aggregate Path with Its Observation Record and the Synthetic Copy's Regularised Path with Its Record); by claim 2 of The Path-Closeness Event under the Cost Bound: Closeness of the Empirical State Measure to the Mean-Field Trajectory and of the Record-Frozen Control to the Mean-Field Control on an Event of Probability 1−O(N−1/2)1-O(N^{-1/2}), ∣Σt(ω)−St∣≤εS(N)|\Sigma_{t}(\omega)-S_{t}|\le\varepsilon_{S}(N) for every t∈[0,T]t\in[0,T], so εS(N)\varepsilon_{S}(N) is an upper bound of the set whose least upper bound is s(Π(ω))\mathsf{s}(\Pi(\omega)), whence s(Π(ω))≤εS(N)\mathsf{s}(\Pi(\omega))\le\varepsilon_{S}(N); and by the same claim with t=st=s and by claim 1(b), d(W(s)(ω))=∫[0,s]∣α^(t,ω)−At∣ dt≤εctl(N)\mathsf{d}(W^{(s)}(\omega))=\int_{[0,s]}|\hat{\alpha}(t,\omega)-A_{t}|\,dt\le\varepsilon_{\mathrm{ctl}}(N). Hence (Π(ω),W(s)(ω))∈E(\Pi(\omega),W^{(s)}(\omega))\in\mathsf{E}, that is, ΩNcl⊆{(Π,W(s))∈E}\Omega^{\mathrm{cl}}_{N}\subseteq\{(\Pi,W^{(s)})\in\mathsf{E}\}, and by monotonicity of PagP^{\mathrm{ag}} and claim 2 of The Path-Closeness Event under the Cost Bound: Closeness of the Empirical State Measure to the Mean-Field Trajectory and of the Record-Frozen Control to the Mean-Field Control on an Event of Probability 1−O(N−1/2)1-O(N^{-1/2}),

πˉnc≤Pag({(Π,W(s))∉E})≤Pag(Ωag∖ΩNcl)≤N−1/2+cQκ♯N−1.\bar\pi^{\mathrm{nc}}\le P^{\mathrm{ag}}\bigl(\{(\Pi,W^{(s)})\notin\mathsf{E}\}\bigr)\le P^{\mathrm{ag}}\bigl(\Omega^{\mathrm{ag}}\setminus\Omega^{\mathrm{cl}}_{N}\bigr)\le N^{-1/2}+c_{Q}\kappa^{\sharp}N^{-1}.

Claim 4. Claims 1 and 2 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 are used below in the present instance, which is legitimate by the scope statement preceding its claim 1, although (FM) and (DM) have not yet been established. Let Qs=(Q∩[0,s])∪{s}\mathsf{Q}_{s}=(\mathbb{Q}\cap[0,s])\cup\{s\}, the countable set of claim 2 of that lemma (countable by The Integers and the Rational Numbers are Countable and claims 3 and 6 of Basic Properties of Countable Sets, and nonempty), so that it is the set of terms of a sequence (tn)n∈N(t_{n})_{n\in\mathbb{N}} by Countable Set; by that claim, eˉ(ω,r)=sup⁡nN ∣Σˉtn♯,r(ω)−Φtnr∣\bar{\mathsf{e}}(\omega,r)=\sup_{n}\sqrt{N}\,|\bar\Sigma^{\sharp,r}_{t_{n}}(\omega)-\Phi^{r}_{t_{n}}|. Define F:Path×Rs→RF:\mathsf{Path}\times\mathbf{R}_{s}\to\mathbb{R} by F(p,r)=sup⁡nfn(p,r)F(p,r)=\sup_{n}f_{n}(p,r) with fn(p,r)=N2∣p(tn)−Φtnr∣4f_{n}(p,r)=N^{2}|p(t_{n})-\Phi^{r}_{t_{n}}|^{4}. Each fnf_{n} is measurable with respect to C⊗Rs\mathcal{C}\otimes\mathcal{R}_{s}: (p,r)↦p(tn)γ(p,r)\mapsto p(t_{n})^{\gamma} is the composition of the projection onto Path\mathsf{Path} with the C\mathcal{C}-measurable map p↦ϕ(p(tn))p\mapsto\phi(p(t_{n})), ϕ(y)=yγ\phi(y)=y^{\gamma}, of claim 1 of The Space of Piecewise Constant Paths in a Finite Set: Measurability of Evaluations, Restrictions, Left Limits, and Occupation Integrals; (p,r)↦Φtnr,γ(p,r)\mapsto\Phi^{r,\gamma}_{t_{n}} is the composition of the projection onto Rs\mathbf{R}_{s} with the Rs\mathcal{R}_{s}-measurable map of claim 1 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; and fnf_{n} is obtained from these by differences, squares, sums and multiplication by N2N^{2} (claims 2 and 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, ∣z∣4=(∑γ(zγ)2)2|z|^{4}=(\sum_{\gamma}(z^{\gamma})^{2})^{2}). Since p(tn)p(t_{n}) and Φtnr\Phi^{r}_{t_{n}} lie in Δl\Delta^{l}, 0≤fn≤16N20\le f_{n}\le16N^{2}, so FF is real-valued and C⊗Rs\mathcal{C}\otimes\mathcal{R}_{s}-measurable by claim 1 of Measurability of Countable Suprema, Bounded Pointwise Limits, Monotone Functions, and Continuous Functions. For a bounded family (an)(a_{n}) of nonnegative reals, (sup⁡nan)4=sup⁡nan4(\sup_{n}a_{n})^{4}=\sup_{n}a_{n}^{4}: each an4≤(sup⁡kak)4a_{n}^{4}\le(\sup_{k}a_{k})^{4}, and conversely each an≤(sup⁡kak4)1/4a_{n}\le(\sup_{k}a_{k}^{4})^{1/4}, so sup⁡nan≤(sup⁡kak4)1/4\sup_{n}a_{n}\le(\sup_{k}a_{k}^{4})^{1/4} and (sup⁡nan)4≤sup⁡kak4(\sup_{n}a_{n})^{4}\le\sup_{k}a_{k}^{4} (monotonicity of fourth powers and fourth roots). Hence F(Πˉ(ω,r),r)=eˉ(ω,r)4F(\bar\Pi(\omega,r),r)=\bar{\mathsf{e}}(\omega,r)^{4}, and on Ω♯\Omega^{\sharp}, eˉ4=F(Π♯,D)\bar{\mathsf{e}}^{4}=F(\Pi^{\sharp},\mathsf{D}). By claim 2 of Law Identity between the N-Agent Aggregate Path with Its Observation Record and the Synthetic Copy's Regularised Path with Its Record with Pag(D0)=1P^{\mathrm{ag}}(D_{0})=1,

∫Ω♯eˉ4 dμ♯=∫Ω♯F(Π♯,D) dμ♯=Eag[1D0F(Π,W(s))]≤Eag[F(Π,W(s))].\int_{\Omega^{\sharp}}\bar{\mathsf{e}}^{4}\,d\mu^{\sharp}=\int_{\Omega^{\sharp}}F(\Pi^{\sharp},\mathsf{D})\,d\mu^{\sharp}=\mathbb{E}^{\mathrm{ag}}\bigl[\mathbf{1}_{D_{0}}F(\Pi,W^{(s)})\bigr]\le\mathbb{E}^{\mathrm{ag}}\bigl[F(\Pi,W^{(s)})\bigr].

For ω∈Ω0ag\omega\in\Omega^{\mathrm{ag}}_{0}: Π(ω)(t)=Σt(ω)\Pi(\omega)(t)=\Sigma_{t}(\omega), and ΦtW(s)(ω)=Φt(s),W(s)(ω)=Φt(ω)\Phi^{W^{(s)}(\omega)}_{t}=\Phi^{(s),W^{(s)}(\omega)}_{t}=\Phi_{t}(\omega) for t∈[0,s]t\in[0,s] by claim 1(a) and claim 3 of The Observation-Centred Fluctuation at an Intermediate Time: Restriction of the Mean-Field Flow and of the Realized Control to a Shorter Horizon, Representation through the Aggregate State and the Record Prefix, and Transport of Its Joint Law with the Record to the Synthetic Copy, so F(Π(ω),W(s)(ω))=sup⁡nN2∣Σtn(ω)−Φtn(ω)∣4≤N2Q(ω)4F(\Pi(\omega),W^{(s)}(\omega))=\sup_{n}N^{2}|\Sigma_{t_{n}}(\omega)-\Phi_{t_{n}}(\omega)|^{4}\le N^{2}Q(\omega)^{4}, because ∣Σt(ω)−Φt(ω)∣≤Q(ω)|\Sigma_{t}(\omega)-\Phi_{t}(\omega)|\le Q(\omega) for every t∈[0,T]t\in[0,T] by The Empirical State Measure Deviates from the Realized Mean-Field Flow by at Most the Noise Majorant, applied in the instance of the setting of Pre-Stopping-Time Envelope and Restricted Moment Bounds for the State Fluctuation Process fixed in the Data of The Path-Closeness Event under the Cost Bound: Closeness of the Empirical State Measure to the Mean-Field Trajectory and of the Record-Frozen Control to the Mean-Field Control on an Event of Probability 1−O(N−1/2)1-O(N^{-1/2}), in which QQ is the noise majorant and the realized mean-field flow is Φ\Phi (formed with the base point S0S_{0}, the initial point of the trajectory of the stationary triple). For ω∉Ω0ag\omega\notin\Omega^{\mathrm{ag}}_{0}, F≤16N2F\le16N^{2}. Hence F(Π,W(s))≤N2Q4+16N21Ωag∖Ω0agF(\Pi,W^{(s)})\le N^{2}Q^{4}+16N^{2}\mathbf{1}_{\Omega^{\mathrm{ag}}\setminus\Omega^{\mathrm{ag}}_{0}} pointwise, and by monotonicity, additivity and positive homogeneity, using Pag(Ωag∖Ω0ag)=0P^{\mathrm{ag}}(\Omega^{\mathrm{ag}}\setminus\Omega^{\mathrm{ag}}_{0})=0 (Ω0ag\Omega^{\mathrm{ag}}_{0} having probability one by Solution of the Controlled N-Agent Dynamics) and claim 1 of The Path-Closeness Event under the Cost Bound: Closeness of the Empirical State Measure to the Mean-Field Trajectory and of the Record-Frozen Control to the Mean-Field Control on an Event of Probability 1−O(N−1/2)1-O(N^{-1/2}),

∫Ω♯eˉ4 dμ♯≤N2 Eag[Q4]≤N2⋅cQκ♯N−2=cQκ♯.\int_{\Omega^{\sharp}}\bar{\mathsf{e}}^{4}\,d\mu^{\sharp}\le N^{2}\,\mathbb{E}^{\mathrm{ag}}[Q^{4}]\le N^{2}\cdot c_{Q}\kappa^{\sharp}N^{-2}=c_{Q}\kappa^{\sharp}.

Thus (FM) holds with c4=cQκ♯\mathsf{c}_{4}=c_{Q}\kappa^{\sharp}, a real number which is nonnegative because it dominates N2Eag[Q4]≥0N^{2}\mathbb{E}^{\mathrm{ag}}[Q^{4}]\ge0.

Claim 5. The concluding statements of claims 2 and 3 of 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 refer to the setting and hypotheses 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; the setting and the hypotheses (OC), (X), (W), (G), (G′'), (CL), (AF), (CP), (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 are those 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 verbatim (the later version adds only the scope statement on its claims 1 and 2, a parenthetical remark inside its claim 1, and the explicit naming of F♯\mathcal{F}^{\sharp} and λd\lambda_{d}, these being the objects already fixed by The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record, so that the setting and hypotheses, and hence the instances, are the same), so those concluding statements apply to the present instance; the concluding statement of claim 3 is what is used below, that of claim 2 being replaced by a direct verification. The setting of 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 is that of The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record, adopted on the copy side, and its claims 1 and 2 require RR to be a natural number, which holds by (L); so for the data w1=wclkw_{1}=\mathsf{w}^{\mathrm{clk}}, w2=μmax⁡w_{2}=\mu_{\max}, x1x_{1}, x2x_{2} its claim 2 furnishes a family (Ξc)c∈L(\Xi^{c})_{c\in\mathcal{L}} of F\mathcal{F}-measurable square-integrable maps Ω→[0,∞)\Omega\to[0,\infty) with Discwclk(P♯,c(ω))+Discμmax⁡(P♯,c(ω))≤Ξc(ω)\mathrm{Disc}_{\mathsf{w}^{\mathrm{clk}}}(\mathsf{P}^{\sharp,c}(\omega))+\mathrm{Disc}_{\mu_{\max}}(\mathsf{P}^{\sharp,c}(\omega))\le\Xi^{c}(\omega) for every ω∈Ω\omega\in\Omega, in particular for every ω∈G\omega\in G, and with the displayed bound on ∥Ξc∥2=(E[(Ξc)2])1/2\lVert\Xi^{c}\rVert_{2}=(\mathbb{E}[(\Xi^{c})^{2}])^{1/2}; here wclk=N(Λ1s εS+εctl)\mathsf{w}^{\mathrm{clk}}=N(\Lambda_{1}s\,\varepsilon_{S}+\varepsilon_{\mathrm{ctl}}) is formed, as in Mean-Square Assembly of the Estimand Linearisation on the Synthetic Copy: Approximation of the Recentred Copy Endpoint by an Affine Function of the Parameter with horizon ss, from the tolerances of claim 3. This is hypothesis (DM) for this family. The present instance of the setting 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 (horizon ss) has the hypotheses (OC), (X), (W), (G), (G′'), (AF) and (CP) by assumption, (CL) by claim 3, (FM) by claim 4 and (DM) as just shown, and its probability space, copy clocks, clock horizon, cells, cell-count vector and bijection are those of 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; hence the concluding statement of claim 3 of that lemma gives k44≤3(∑qαq2μq)2+∑qαq4μq\mathsf{k}_{4}^{4}\le3(\sum_{q}\alpha_{q}^{2}\mu_{q})^{2}+\sum_{q}\alpha_{q}^{4}\mu_{q} for the cell coefficients α\alpha of the adopted setting. All hypotheses 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 being satisfied, its claim 4 gives ∥α⋅Θ+ς(D)−c⋅X′′∥2≤e1+⋯+e5\lVert\alpha\cdot\Theta+\varsigma(\mathsf{D})-\mathbf{c}\cdot X''\rVert_{2}\le\mathsf{e}_{1}+\dots+\mathsf{e}_{5} with its constants formed from the present data: e1=∣c∣Φˉ2N∣x0−z0∣\mathsf{e}_{1}=|\mathbf{c}|\bar\Phi^{2}\sqrt{N}|\mathsf{x}_{0}-z_{0}| with z0=S0z_{0}=S_{0}; e2\mathsf{e}_{2} with the horizon ss, c4=cQκ♯\mathsf{c}_{4}=c_{Q}\kappa^{\sharp}, εS=εS(N)\varepsilon_{S}=\varepsilon_{S}(N) and εctl=CLipεctl(N)\varepsilon_{\mathrm{ctl}}=C_{\mathrm{Lip}}\varepsilon_{\mathrm{ctl}}(N), which is the displayed expression; e3\mathsf{e}_{3} with (E[(Ξc)2])1/2=∥Ξc∥2(\mathbb{E}[(\Xi^{c})^{2}])^{1/2}=\lVert\Xi^{c}\rVert_{2}; e4=η∣α∣\mathsf{e}_{4}=\sqrt{\eta}|\alpha|; and e5=2(g1/4+(πˉnc)1/4)(∣c∣c41/4+k4/N)\mathsf{e}_{5}=\sqrt{2}(\mathsf{g}^{1/4}+(\bar\pi^{\mathrm{nc}})^{1/4})(|\mathbf{c}|\mathsf{c}_{4}^{1/4}+\mathsf{k}_{4}/\sqrt{N}), which is at most e^5\hat{\mathsf{e}}_{5} because 0≤πˉnc≤N−1/2+cQκ♯N−10\le\bar\pi^{\mathrm{nc}}\le N^{-1/2}+c_{Q}\kappa^{\sharp}N^{-1} by claim 3, fourth roots are monotone, and the second factor is nonnegative; this gives the second inequality of the display. Finally, c⋅X′′\mathbf{c}\cdot X'' is the function (ω,θ,r)↦c⋅X′′(ω,r)=c⋅Xs′′(ω,θ,r)(\omega,\theta,r)\mapsto\mathbf{c}\cdot X''(\omega,r)=\mathbf{c}\cdot X''_{s}(\omega,\theta,r) on Ω♯\Omega^{\sharp} by claim 1(a), which identifies the left-hand side as stated.

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