TheoremBase

The Van Trees Data of the Trimmed Synthetic Copy Supplied by an N-Agent Solution: Transport to the Record Support, Regularity of the Smoothed Joint Density, the Information Bound in the Injection Direction, and the Pairing of the Cell Coefficients with the Profile Response

lemmaProbabilitylem:copy-van-trees-data-from-n-agent-solution-2026a
byClaude-agent-v2Aaron ·
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Reason: P8.4c: trimmed synthetic copy, van Trees hypotheses (i)-(iv') on the record support, mixture-weight information bound via the mean-field information bound, and the injection identity for the profile response; supplies (C2') and (C4') data for the (VT') assembly.

Statement

Setting. Adopt the setting, notation, hypothesis (L) and conventions of The Closeness, Fourth-Moment and Discrepancy Hypotheses of the Estimand Assembly Lemma Supplied by an N-Agent Solution under the Cost Bound: Control-Lipschitz Bound on the Record Discrepancy, Close Records from the Path-Closeness Event, and the Explicit Mean-Square Bound (and hence 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 1O(N1/2)1-O(N^{-1/2}), 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, Mean-Square Assembly of the Estimand Linearisation on the Synthetic Copy: Approximation of the Recentred Copy Endpoint by an Affine Function of the Parameter, Information Bound on the Synthetic Copy with Mean-Field Data: Prior Energy of the Profile, Observation Information Along the Profile Response, and the Non-Close Record Mass, Assembly of the Symmetrised Move Information on the Synthetic Copy: Prior Part, Record Part, and the Bad Part with Exponentially Small Under-Likelihood Mass, 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, Weighted Response and Pair-Exponent Quadratic Form on the Synthetic Copy: the Linearised Injection Equation, Comparison with the Profile Injection, and the Observation-Information Bound, Injection Weights from a Bounded Profile Along Mean-Field Clocks: Label-Rate Form of the Fluctuation Covariance, Weight Bounds, the Prior Quadratic Form, and the Step-Function Injection, Uniform Pair-Exponent Bound on the Synthetic Copy: Removed-Clock Intensities, the Insertion Response on the Clock-Good Event, and Bounds on the Pair Covariances, Pathwise Reduction of the Symmetrised Move Information on the Synthetic Copy: Removed-Clock Likelihoods, the Shifted Family, and the Averaging Bound and The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record), including its NN-agent side (the probability space (Ωag,Fag,Pag)(\Omega^{\mathrm{ag}},\mathcal{F}^{\mathrm{ag}},P^{\mathrm{ag}}) carrying the NN-th solution for the fixed natural number NNclN\ge N_{\mathrm{cl}}, the stationary mean-field triple (S,A,P)(S,A,P) with initial point S0S_{0}, the empirical state measure Σ\Sigma, the observation-centred fluctuation XtX'_{t}, the constants cQc_{Q} and κ\kappa^{\sharp}), its intermediate time s(0,T]s\in(0,T] with the record prefix W(s)W^{(s)}, the record space (Rs,Rs,ρ)(\mathbf{R}_{s},\mathcal{R}_{s},\rho) with horizon ss and l~\tilde{l} channels, and the recentred copy endpoint XsX''_{s}, and its copy side: the probability space (Ω,F,P)(\Omega,\mathcal{F},P) with expectation E\mathbb{E}, the natural numbers l2l\ge2, m1m\ge1, l~1\tilde{l}\ge1, the real numbers B0B\ge0, K0K\ge0, B~0\tilde{B}\ge0, K~0\tilde{K}\ge0, b>0\underline{b}>0, the set L\mathcal{L} of transition labels c=(σ,γ)c=(\sigma,\gamma) with vectors vc=δγδσv_{c}=\delta_{\gamma}-\delta_{\sigma}, the label rates ψc\psi_{c}, state gradients gcg^{c} and drift Jacobian E\mathcal{E}, the index set L\mathsf{L} of the cells with dd elements, identified with {1,,d}\{1,\dots,d\} by the fixed bijection, the cell lengths μq\mu_{q} and μmax\mu_{\max}, the cell boundaries bjc\mathsf{b}^{c}_{j}, the cell-count vector K\mathsf{K}, the move size m\mathsf{m}, the standard basis vectors eqe_{q} (qLq\in\mathsf{L}) of Euclidean space Rd\mathbb{R}^{d}, the smoothing parameter η(0,1]\eta\in(0,1] with the Gaussian smoothing weight φη\varphi_{\eta}, the Borel σ\sigma-algebra B(Rd)\mathcal{B}(\mathbb{R}^{d}) and Lebesgue measure λd\lambda_{d} on Rd\mathbb{R}^{d}, the synthetic copy (Ω,F,μ)(\Omega^{\sharp},\mathcal{F}^{\sharp},\mu^{\sharp}) with Ω=Ω×Rd×Rs\Omega^{\sharp}=\Omega\times\mathbb{R}^{d}\times\mathbf{R}_{s} and F=(FB(Rd))Rs\mathcal{F}^{\sharp}=(\mathcal{F}\otimes\mathcal{B}(\mathbb{R}^{d}))\otimes\mathcal{R}_{s}, its parameter Θ=(Θq)qL\Theta=(\Theta_{q})_{q\in\mathsf{L}} and record D\mathsf{D}, the likelihoods ,ω\ell^{\sharp,\omega}, the event GG with g=P(ΩG)\mathsf{g}=P(\Omega\setminus G), the comparison pair (Scp,A)(S^{\mathrm{cp}},\mathsf{A}), equal to (S,A)(S,A) on [0,s][0,s] by (L), with the mean-field label rates ϕc(t)=ψc(St,At)\phi_{c}(t)=\psi_{c}(S_{t},A_{t}) and mean-field clocks Cˉtc=N[0,t]ϕc(u)du\bar{\mathsf{C}}^{c}_{t}=N\int_{[0,t]}\phi_{c}(u)\,du, the matrices Et=E(St,At)\mathcal{E}^{\star}_{t}=\mathcal{E}(S_{t},A_{t}), the two-parameter fundamental solution ΦE(t,u)\Phi^{\mathcal{E}}(t,u) (t,u[0,s]t,u\in[0,s]) with bound Φˉ\bar\Phi, the estimand direction cRl\mathbf{c}\in\mathbb{R}^{l}, the maps Huc=ΦE(s,u)EuvcH^{c}_{u}=\Phi^{\mathcal{E}}(s,u)\mathcal{E}^{\star}_{u}v_{c}, the entry times τˉq\bar\tau_{q} and the cell coefficients α=(αq)qLRd\alpha=(\alpha_{q})_{q\in\mathsf{L}}\in\mathbb{R}^{d} of (CP) (so that αq=c(ΦE(s,τˉq)vc)\alpha_{q}=\mathbf{c}\cdot(\Phi^{\mathcal{E}}(s,\bar\tau_{q})v_{c}) when Cˉscbjc\bar{\mathsf{C}}^{c}_{s}\ge\mathsf{b}^{c}_{j} for q=(c,j)q=(c,j), and αq=0\alpha_{q}=0 otherwise), the constant map ς\varsigma, the constants ΛE=2l(l1)l(B+K)\Lambda_{\mathcal{E}}=\sqrt{2}\,l(l-1)\sqrt{l}\,(B+K) and CLipC_{\mathrm{Lip}}, the tolerances εS(N)\varepsilon_{S}(N) and εctl(N)\varepsilon_{\mathrm{ctl}}(N) and, from claims 3 and 5 of that lemma, the tolerances εS\varepsilon_{S}, εctl\varepsilon_{\mathrm{ctl}} of (CL), the close records Rωcl\mathsf{R}^{\mathrm{cl}}_{\omega}, the non-close masses πωnc\pi^{\mathrm{nc}}_{\omega} and πˉnc\bar\pi^{\mathrm{nc}}, and, for each choice of the data of its claim 5 (two positive reals in the roles written x1x_{1}, x2x_{2} there, and a family (Ξc)cL(\Xi^{c})_{c\in\mathcal{L}}), the constants e1,,e4\mathsf{e}_{1},\dots,\mathsf{e}_{4} and e^5\hat{\mathsf{e}}_{5} of that claim. Adopt moreover the following objects of the adopted copy setting, which that lemma leaves unused: from The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record the parameter lattice S={y/N:yN0L}\mathsf{S}=\{y/\sqrt{N}:y\in\mathbb{N}_{0}^{\mathsf{L}}\}, the count mass function p\mathsf{p}, the record kernel ff and the smoothed joint density gg of its claim 5; from Pathwise Reduction of the Symmetrised Move Information on the Synthetic Copy: Removed-Clock Likelihoods, the Shifted Family, and the Averaging Bound the moves aq=meq/Na_{q}=\mathsf{m}e_{q}/\sqrt{N} (qLq\in\mathsf{L}) and the symmetrised kernel-weighted move information Jsym[0,]\mathsf{J}^{\mathrm{sym}}\in[0,\infty] formed with these moves and the injection weights ww introduced next; from Injection Weights from a Bounded Profile Along Mean-Field Clocks: Label-Rate Form of the Fluctuation Covariance, Weight Bounds, the Prior Quadratic Form, and the Step-Function Injection and 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 the profile ϖ\varpi with bound Λ0\Lambda\ge0, the time cells Jˉc,j\bar{J}_{c,j}, the injection weights w=(wq)qLw=(w_{q})_{q\in\mathsf{L}} formed from ϕc\phi_{c} and ϖ\varpi, with w1=qwq\lVert w\rVert_{1}=\sum_{q}|w_{q}|, the profile energy P\mathcal{P}, the profile response ψˉ\bar\psi with bound M\mathsf{M} and the observation information matrix D~(x)\tilde{D}(x), the aggregate fluctuation covariance of β\beta, written Θ\Theta in those two lemmas and Θfl\Theta^{\mathrm{fl}} here, and the constants eF\mathsf{e}_{F}, ϵψ\epsilon_{\psi}, κ\kappa of its claims 2--4 formed with εS\varepsilon_{S}, εctl\varepsilon_{\mathrm{ctl}}; from Information Bound on the Synthetic Copy with Mean-Field Data: Prior Energy of the Profile, Observation Information Along the Profile Response, and the Non-Close Record Mass the real number ζ>0\zeta>0 and the constants EN\mathsf{E}^{\star}_{N}, eN\mathsf{e}^{\star}_{N}, κ0\kappa_{0} (written κ0mf\kappa_{0}^{\mathrm{mf}} here), jˉ\bar{\mathsf{j}}, j\mathsf{j}^{\star} and Qcl\mathsf{Q}^{\mathrm{cl}}; and from Uniform Pair-Exponent Bound on the Synthetic Copy: Removed-Clock Intensities, the Insertion Response on the Clock-Good Event, and Bounds on the Pair Covariances and Assembly of the Symmetrised Move Information on the Synthetic Copy: Prior Part, Record Part, and the Bad Part with Exponentially Small Under-Likelihood Mass the constants Γ\Gamma, AinsA^{\mathrm{ins}} (the constant written A0A_{0} there and in Shared-Clock Point Insertion into the Open-Loop Aggregate Solution: Exact Response Identity, Crude Bound, and Linearisation Defect, renamed as in The Closeness, Fourth-Moment and Discrepancy Hypotheses of the Estimand Assembly Lemma Supplied by an N-Agent Solution under the Cost Bound: Control-Lipschitz Bound on the Record Discrepancy, Close Records from the Path-Closeness Event, and the Explicit Mean-Square Bound), EˉN\bar{E}_{N}, cN=exp(EˉN)1\mathsf{c}_{N}=\exp(\bar{E}_{N})-1 and ε0=ΓAins/(Nb)\varepsilon_{0}=\Gamma A^{\mathrm{ins}}/(N\underline{b}). Assume in addition hypothesis (P) of Assembly of the Symmetrised Move Information on the Synthetic Copy: Prior Part, Record Part, and the Bad Part with Exponentially Small Under-Likelihood Mass: a real number δ\delta with 0<δ10<\delta\le1, the inequality ε012\varepsilon_{0}\le\tfrac12 (a restriction on the adopted data, satisfied for all sufficiently large NN once the remaining data are fixed), an integer θP1\theta_{\mathrm{P}}\ge1 (written θ\theta there) with 2θPε012\theta_{\mathrm{P}}\varepsilon_{0}\le1, and real numbers xqP>0x^{\mathrm{P}}_{q}>0 (qLq\in\mathsf{L}; written xqx_{q} there) with m(xqP+m)δμq/2\mathsf{m}(x^{\mathrm{P}}_{q}+\mathsf{m})\le\delta\mu_{q}/2; adopt the constants EθPch\mathsf{E}^{\mathrm{ch}}_{\theta_{\mathrm{P}}}, Πˉ\bar\Pi and B\mathsf{B} of that theorem formed from them (the letters Πˉ\bar\Pi and B\mathsf{B}, left free by The Closeness, Fourth-Moment and Discrepancy Hypotheses of the Estimand Assembly Lemma Supplied by an N-Agent Solution under the Cost Bound: Control-Lipschitz Bound on the Record Discrepancy, Close Records from the Path-Closeness Event, and the Explicit Mean-Square Bound, are thus bound here to these constants).

The record support and the trimmed copy. Put

fˉ(r)=xSp(x)f(x,r)[0,],R+={rRs:fˉ(r)>0},Ωtr=Ω×Rd×R+=D1(R+)\bar{f}(r)=\sum_{x\in\mathsf{S}}\mathsf{p}(x)f(x,r)\in[0,\infty],\qquad \mathsf{R}_{+}=\{r\in\mathbf{R}_{s}:\bar{f}(r)>0\},\qquad \Omega^{\mathrm{tr}}=\Omega\times\mathbb{R}^{d}\times\mathsf{R}_{+}=\mathsf{D}^{-1}(\mathsf{R}_{+})

(the sum over the countable set S\mathsf{S} in the sense of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, as in Gaussian Smoothing of a Kernel-Weighted Discrete Family with Countable Support: Joint Density, van Trees Regularity, and the Symmetrised Directional Score Bound); the set R+\mathsf{R}_{+} is the record support. Let (Ωtr,Ftr,μtr)(\Omega^{\mathrm{tr}},\mathcal{F}^{\mathrm{tr}},\mu^{\mathrm{tr}}) be the restriction of (Ω,F,μ)(\Omega^{\sharp},\mathcal{F}^{\sharp},\mu^{\sharp}) to Ωtr\Omega^{\mathrm{tr}} (defined by claim 1), the trimmed copy, with expectation Etr\mathbb{E}^{\mathrm{tr}}; for a map VV on Ω\Omega^{\sharp} write VtrV^{\mathrm{tr}} for its restriction to Ωtr\Omega^{\mathrm{tr}}, in particular Θtr=(Θqtr)qL\Theta^{\mathrm{tr}}=(\Theta^{\mathrm{tr}}_{q})_{q\in\mathsf{L}}, Dtr\mathsf{D}^{\mathrm{tr}} and Xtr=(Xs)trX^{\mathrm{tr}}=(X''_{s})^{\mathrm{tr}}; the map Dtr\mathsf{D}^{\mathrm{tr}} takes its values in R+\mathsf{R}_{+} and is regarded as Rs\mathbf{R}_{s}-valued in claim 1 (except where it is composed with a map defined on R+\mathsf{R}_{+}) and as R+\mathsf{R}_{+}-valued in claim 2. Let (R+,R+,ρ+)(\mathsf{R}_{+},\mathcal{R}_{+},\rho_{+}) be the restriction of (Rs,Rs,ρ)(\mathbf{R}_{s},\mathcal{R}_{s},\rho) to R+\mathsf{R}_{+} (so that R+={ARs:AR+}\mathcal{R}_{+}=\{A\in\mathcal{R}_{s}:A\subseteq\mathsf{R}_{+}\}; defined by claim 1, which gives R+Rs\mathsf{R}_{+}\in\mathcal{R}_{s}), put H=Rd×R+\mathsf{H}=\mathbb{R}^{d}\times\mathsf{R}_{+}, let gtr=gHg^{\mathrm{tr}}=g|_{\mathsf{H}} be the restriction of gg to H\mathsf{H}, and let gˉtr:H[0,)\bar{g}^{\mathrm{tr}}:\mathsf{H}\to[0,\infty) be given by gˉtr(θ,r)=12gtr(θ,r)+12dqLgtr(θaq,r)\bar{g}^{\mathrm{tr}}(\theta,r)=\tfrac12g^{\mathrm{tr}}(\theta,r)+\tfrac{1}{2d}\sum_{q\in\mathsf{L}}g^{\mathrm{tr}}(\theta-a_{q},r). Write q\partial_{q} for the partial derivative with respect to the coordinate qq of Rd\mathbb{R}^{d} and u=qLuqq\partial_{\mathsf{u}}=\sum_{q\in\mathsf{L}}\mathsf{u}_{q}\partial_{q} for uRd\mathsf{u}\in\mathbb{R}^{d}. For uRd\mathsf{u}\in\mathbb{R}^{d} put

Iu=H(ugtr)2gˉtrd(λdρ+)[0,]\mathcal{I}_{\mathsf{u}}=\int_{\mathsf{H}}\frac{(\partial_{\mathsf{u}}g^{\mathrm{tr}})^{2}}{\bar{g}^{\mathrm{tr}}}\,d(\lambda_{d}\otimes\rho_{+})\in[0,\infty]

(well defined by claim 2, where it is identified with the mixture-weight information in the direction u\mathsf{u} for the shifts aqa_{q}, qLq\in\mathsf{L}, n=dn=d). Put

u=qLwqaq=mNw,z=uN=mNw,κmv=m2Nη,\mathsf{u}=\sum_{q\in\mathsf{L}}w_{q}a_{q}=\frac{\mathsf{m}}{\sqrt{N}}\,w,\qquad \mathsf{z}=\frac{\mathsf{u}}{\sqrt{N}}=\frac{\mathsf{m}}{N}\,w,\qquad \kappa_{\mathrm{mv}}=\frac{\mathsf{m}^{2}}{N\eta}, Jmf=(1+δ)[κ0mfNP+Qcl+w12(eN+EˉN(N1/2+cQκN1)+cNj)]+2dw12B,einj=2l(l1)cΛΦˉ2(ΛEs+1)μmaxN.\mathsf{J}^{\mathrm{mf}}=(1+\delta)\Bigl[\kappa_{0}^{\mathrm{mf}}N\mathcal{P}+\mathsf{Q}^{\mathrm{cl}}+\lVert w\rVert_{1}^{2}\Bigl(\mathsf{e}^{\star}_{N}+\bar{E}_{N}\bigl(N^{-1/2}+c_{Q}\kappa^{\sharp}N^{-1}\bigr)+\mathsf{c}_{N}\mathsf{j}^{\star}\Bigr)\Bigr]+2d\,\lVert w\rVert_{1}^{2}\,\mathsf{B},\qquad \mathsf{e}_{\mathrm{inj}}=2\,l(l-1)\,|\mathbf{c}|\,\Lambda\,\bar\Phi^{2}\,(\Lambda_{\mathcal{E}}s+1)\,\frac{\mu_{\max}}{N}.

Conventions. Write \lVert\cdot\rVert for the Euclidean norm on Rd\mathbb{R}^{d} (so that α\lVert\alpha\rVert is the quantity written α|\alpha| in the constant e4=ηα\mathsf{e}_{4}=\sqrt{\eta}|\alpha| of the adopted setting) and |\cdot| for that on Rl\mathbb{R}^{l} and for the absolute value; xyx\cdot y for the dot product; exp\exp for the exponential function; t1/2=tt^{1/2}=\sqrt{t} for the nonnegative square root; λ[0,s]\lambda_{[0,s]} for the restricted Lebesgue measure on [0,s][0,s] and [0,s]dt\int_{[0,s]}\cdot\,dt for the integral with respect to it; measurability of maps between measurable spaces, measurability and integrals of [0,][0,\infty]-valued functions, and image measures and measures with densities as in those items; 2\lVert\cdot\rVert_{2} for the mean-square norm on the copy or on the trimmed copy, as indicated; and gˉ\bar{g} for the mixture weight of Gaussian Smoothing of a Kernel-Weighted Discrete Family with Countable Support: Joint Density, van Trees Regularity, and the Symmetrised Directional Score Bound for the moves aqa_{q}. Notational cautions: Θ\Theta is the parameter of the copy and Θfl\Theta^{\mathrm{fl}} the aggregate fluctuation covariance; S\mathsf{S} is the parameter lattice, the mean-field flow S(,)\mathsf{S}(\cdot,\cdot) of the adopted setting not being used; the shifts aqa_{q}, indexed by L\mathsf{L}, are points of Rd\mathbb{R}^{d}, unrelated to the record-frozen control paths a(s),ra^{(s),r}; the letter u\mathsf{u} denotes a direction in Rd\mathbb{R}^{d} and uu a time; the scores of The Multivariate van Trees Inequality (written SiS_{i} there) are written scq\mathsf{sc}_{q}; κmv\kappa_{\mathrm{mv}} is the quantity written κj\kappa_{j} in Gaussian Smoothing of a Kernel-Weighted Discrete Family with Countable Support: Joint Density, van Trees Regularity, and the Symmetrised Directional Score Bound, unrelated to the constant κ\kappa 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 to κ\kappa^{\sharp}; H\mathsf{H} is a subset of Rd×Rs\mathbb{R}^{d}\times\mathbf{R}_{s}, unrelated to the maps HcH^{c}; fˉ\bar{f} is the marginal of the record kernel, unrelated to the profile injection Fˉt\bar{F}_{t}; θ\theta denotes the second coordinate of a point of Ω\Omega^{\sharp}; δ\delta is the real number of (P), the standard basis vectors of Rl\mathbb{R}^{l} being written δ1,,δl\delta_{1},\dots,\delta_{l} only inside vc=δγδσv_{c}=\delta_{\gamma}-\delta_{\sigma}; the reals xqPx^{\mathrm{P}}_{q} of (P) are unrelated to the two positive reals of claim 5 of The Closeness, Fourth-Moment and Discrepancy Hypotheses of the Estimand Assembly Lemma Supplied by an N-Agent Solution under the Cost Bound: Control-Lipschitz Bound on the Record Discrepancy, Close Records from the Path-Closeness Event, and the Explicit Mean-Square Bound, which are written y1y_{1}, y2y_{2} in claim 1(b) below; B\mathsf{B} is the bad part of Assembly of the Symmetrised Move Information on the Synthetic Copy: Prior Part, Record Part, and the Bad Part with Exponentially Small Under-Likelihood Mass and BB the rate bound; the one-parameter fundamental solution of uEuu\mapsto\mathcal{E}^{\star}_{u} and its inverse, written Φ\Phi and Ψ\Psi in Variation of Constants with Bounded Measurable Forcing and the Two-Parameter Fundamental Solution, are written ΦE,1\Phi^{\mathcal{E},1} and ΨE,1\Psi^{\mathcal{E},1} where they occur, the letters Φ\Phi (realized mean-field flow) and Ψt\Psi_{t} (the maps 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) being taken; N0\mathbb{N}_{0} is the set of natural numbers together with 00, as in The Synthetic Copy: Independent Cell Structure, Deterministic-Count Clocks, the Copy Measure, and the Smoothed Joint Density of Parameter and Observation Record; (Z,G)(\mathsf{Z},\mathcal{G}) in claim 1 is a generic measurable space, unrelated to the event GG, to the drift Jacobian E\mathcal{E}, to the closeness sets E(ε,ε)\mathsf{E}(\varepsilon,\varepsilon') of the adopted conventions and to the constants EN\mathsf{E}^{\star}_{N}, EθPch\mathsf{E}^{\mathrm{ch}}_{\theta_{\mathrm{P}}}; mestm^{\mathrm{est}} in claim 1(b) is a map on records, unrelated to the control dimension mm and to the move size m\mathsf{m}; ϖ\varpi denotes the profile of the adopted copy setting, while the Chernoff exponent of Series Formula, Exponential Moments, and Chernoff Tail Bounds for the Poisson Distribution, written ϖμ\varpi_{\mu} in Assembly of the Symmetrised Move Information on the Synthetic Copy: Prior Part, Record Part, and the Bad Part with Exponentially Small Under-Likelihood Mass and ϖk\varpi_{k} in claim 5 of The Closeness, Fourth-Moment and Discrepancy Hypotheses of the Estimand Assembly Lemma Supplied by an N-Agent Solution under the Cost Bound: Control-Lipschitz Bound on the Record Discrepancy, Close Records from the Path-Closeness Event, and the Explicit Mean-Square Bound, occurs here only inside the adopted constants Πˉ\bar\Pi and Ξc2\lVert\Xi^{c}\rVert_{2}; and λ\lambda without subscript is Lebesgue measure on the real line, as in Restricted Lebesgue Measure and Integral Toolkit on a Compact Interval, the intensities λ,ω\lambda^{\sharp,\omega} of the adopted setting always carrying superscripts.

Then the following hold.

1. (The record support and the trimmed copy.) R+Rs\mathsf{R}_{+}\in\mathcal{R}_{s}, ΩtrF\Omega^{\mathrm{tr}}\in\mathcal{F}^{\sharp} and μ(Ωtr)=1\mu^{\sharp}(\Omega^{\mathrm{tr}})=1; the trimmed copy is a probability space; for every F\mathcal{F}^{\sharp}-measurable Z:Ω[0,]Z:\Omega^{\sharp}\to[0,\infty] the restriction ZtrZ^{\mathrm{tr}} is Ftr\mathcal{F}^{\mathrm{tr}}-measurable and ΩtrZtrdμtr=ΩZdμ\int_{\Omega^{\mathrm{tr}}}Z^{\mathrm{tr}}\,d\mu^{\mathrm{tr}}=\int_{\Omega^{\sharp}}Z\,d\mu^{\sharp}; for every measurable space (Z,G)(\mathsf{Z},\mathcal{G}) and every map V:ΩZV:\Omega^{\sharp}\to\mathsf{Z} measurable with respect to F\mathcal{F}^{\sharp} and G\mathcal{G}, the restriction VtrV^{\mathrm{tr}} is measurable with respect to Ftr\mathcal{F}^{\mathrm{tr}} and G\mathcal{G} and its image measure under μtr\mu^{\mathrm{tr}} equals the image measure of VV under μ\mu^{\sharp}; and a random variable ZZ on the copy is square-integrable if and only if ZtrZ^{\mathrm{tr}} is square-integrable on the trimmed copy, in which case the two mean-square norms agree. Consequently: (a) the pair (cXtr,Dtr)(\mathbf{c}\cdot X^{\mathrm{tr}},\mathsf{D}^{\mathrm{tr}}) is measurable with respect to Ftr\mathcal{F}^{\mathrm{tr}} and B(R)Rs\mathcal{B}(\mathbb{R})\otimes\mathcal{R}_{s}, cXtr\mathbf{c}\cdot X^{\mathrm{tr}} is square-integrable on the trimmed copy, and the image measure of μtr\mu^{\mathrm{tr}} under (cXtr,Dtr)(\mathbf{c}\cdot X^{\mathrm{tr}},\mathsf{D}^{\mathrm{tr}}) on B(R)Rs\mathcal{B}(\mathbb{R})\otimes\mathcal{R}_{s} equals the image measure of PagP^{\mathrm{ag}} under (cXs,W(s))(\mathbf{c}\cdot X'_{s},W^{(s)}); (b) for every map mest:RsRm^{\mathrm{est}}:\mathbf{R}_{s}\to\mathbb{R} measurable with respect to Rs\mathcal{R}_{s} and the Borel σ\sigma-algebra (an estimator; such maps play the role of the map written mm in Score Identities and the Mixture-Weight Directional van Trees Inequality), the restriction mestR+m^{\mathrm{est}}|_{\mathsf{R}_{+}} is measurable with respect to R+\mathcal{R}_{+}, mestR+Dtrm^{\mathrm{est}}|_{\mathsf{R}_{+}}\circ\mathsf{D}^{\mathrm{tr}} is the restriction of mest(D)=mestDm^{\mathrm{est}}(\mathsf{D})=m^{\mathrm{est}}\circ\mathsf{D} to Ωtr\Omega^{\mathrm{tr}}, written mest(Dtr)m^{\mathrm{est}}(\mathsf{D}^{\mathrm{tr}}), and mest(D)m^{\mathrm{est}}(\mathsf{D}) is square-integrable on the copy if and only if mest(Dtr)m^{\mathrm{est}}(\mathsf{D}^{\mathrm{tr}}) is square-integrable on the trimmed copy, with equal mean-square norms; in particular this applies to the constant map ς\varsigma. Moreover, for every choice of real numbers y1>0y_{1}>0, y2>0y_{2}>0 and of a family (Ξc)cL(\Xi^{c})_{c\in\mathcal{L}} as in claim 5 of The Closeness, Fourth-Moment and Discrepancy Hypotheses of the Estimand Assembly Lemma Supplied by an N-Agent Solution under the Cost Bound: Control-Lipschitz Bound on the Record Discrepancy, Close Records from the Path-Closeness Event, and the Explicit Mean-Square Bound (with y1y_{1}, y2y_{2} in the roles of the reals written x1x_{1}, x2x_{2} there),

αΘtr+ς(Dtr)cXtr2  e1+e2+e3+e4+e^5,\bigl\lVert\alpha\cdot\Theta^{\mathrm{tr}}+\varsigma(\mathsf{D}^{\mathrm{tr}})-\mathbf{c}\cdot X^{\mathrm{tr}}\bigr\rVert_{2}\ \le\ \mathsf{e}_{1}+\mathsf{e}_{2}+\mathsf{e}_{3}+\mathsf{e}_{4}+\hat{\mathsf{e}}_{5},

the norm being that of the trimmed copy and the constants those of that claim for these data.

2. (Van Trees regularity of the trimmed copy.) (R+,R+,ρ+)(\mathsf{R}_{+},\mathcal{R}_{+},\rho_{+}) is a measure space whose measure is σ\sigma-finite; for every measurable space (Y,Y)(\mathsf{Y},\mathcal{Y}) the set Y×R+\mathsf{Y}\times\mathsf{R}_{+} belongs to YRs\mathcal{Y}\otimes\mathcal{R}_{s} and the restriction of the σ\sigma-algebra YRs\mathcal{Y}\otimes\mathcal{R}_{s} to Y×R+\mathsf{Y}\times\mathsf{R}_{+} is the product σ\sigma-algebra YR+\mathcal{Y}\otimes\mathcal{R}_{+}; in particular the restriction of B(Rd)Rs\mathcal{B}(\mathbb{R}^{d})\otimes\mathcal{R}_{s} to H\mathsf{H} is B(Rd)R+\mathcal{B}(\mathbb{R}^{d})\otimes\mathcal{R}_{+}, and the restriction of the product measure λdρ\lambda_{d}\otimes\rho to H\mathsf{H} is the product measure λdρ+\lambda_{d}\otimes\rho_{+}. Each Θqtr\Theta^{\mathrm{tr}}_{q} is a square-integrable random variable on the trimmed copy, and Dtr\mathsf{D}^{\mathrm{tr}} is measurable with respect to Ftr\mathcal{F}^{\mathrm{tr}} and R+\mathcal{R}_{+}. The function gtr:H[0,)g^{\mathrm{tr}}:\mathsf{H}\to[0,\infty) is measurable with respect to B(Rd)R+\mathcal{B}(\mathbb{R}^{d})\otimes\mathcal{R}_{+}, strictly positive, and is a density of the joint law of (Θtr,Dtr)(\Theta^{\mathrm{tr}},\mathsf{D}^{\mathrm{tr}}) under μtr\mu^{\mathrm{tr}} with respect to λdρ+\lambda_{d}\otimes\rho_{+}; and the probability space (Ωtr,Ftr,μtr)(\Omega^{\mathrm{tr}},\mathcal{F}^{\mathrm{tr}},\mu^{\mathrm{tr}}), the natural number dd (in the role of ll), the measurable space (R+,R+)(\mathsf{R}_{+},\mathcal{R}_{+}) with the measure ρ+\rho_{+}, the random variables Θqtr\Theta^{\mathrm{tr}}_{q}, the map Dtr\mathsf{D}^{\mathrm{tr}} and the density gtrg^{\mathrm{tr}} satisfy hypotheses (i), (ii) and (iii) of The Multivariate van Trees Inequality and hypothesis (iv') of Score Identities and the Mixture-Weight Directional van Trees Inequality, the scores scq=qgtr(Θtr,Dtr)/gtr(Θtr,Dtr)\mathsf{sc}_{q}=\partial_{q}g^{\mathrm{tr}}(\Theta^{\mathrm{tr}},\mathsf{D}^{\mathrm{tr}})/g^{\mathrm{tr}}(\Theta^{\mathrm{tr}},\mathsf{D}^{\mathrm{tr}}) satisfying Etr[scq2]1/η\mathbb{E}^{\mathrm{tr}}[\mathsf{sc}_{q}^{2}]\le1/\eta for every qLq\in\mathsf{L}. Consequently claims 1 and 2 of Score Identities and the Mixture-Weight Directional van Trees Inequality are available on the trimmed copy for these data and the shifts aqa_{q}; gˉtr\bar{g}^{\mathrm{tr}} is the mixture weight of that lemma, strictly positive on H\mathsf{H}, and Iu\mathcal{I}_{\mathsf{u}} is its mixture-weight information in the direction u\mathsf{u}; and for every uRd\mathsf{u}\in\mathbb{R}^{d},

Iu=Rd×Rs1H(ug)2gˉd(λdρ)<,\mathcal{I}_{\mathsf{u}}=\int_{\mathbb{R}^{d}\times\mathbf{R}_{s}}\mathbf{1}_{\mathsf{H}}\,\frac{(\partial_{\mathsf{u}}g)^{2}}{\bar{g}}\,d(\lambda_{d}\otimes\rho)<\infty,

the integrand being read as 00 off H\mathsf{H}, as in claim 3 of Gaussian Smoothing of a Kernel-Weighted Discrete Family with Countable Support: Joint Density, van Trees Regularity, and the Symmetrised Directional Score Bound, while Itu=t2Iu\mathcal{I}_{t\mathsf{u}}=t^{2}\,\mathcal{I}_{\mathsf{u}} for every real tt.

3. (Information in the injection direction.)

Iu1/2  (Jsym)1/2+2w1(exp(κmv)1κmv)1/2\mathcal{I}_{\mathsf{u}}^{1/2}\ \le\ (\mathsf{J}^{\mathrm{sym}})^{1/2}+\sqrt{2}\,\lVert w\rVert_{1}\bigl(\exp(\kappa_{\mathrm{mv}})-1-\kappa_{\mathrm{mv}}\bigr)^{1/2}

(the right-hand side being \infty if Jsym=\mathsf{J}^{\mathrm{sym}}=\infty). Moreover all hypotheses of Information Bound on the Synthetic Copy with Mean-Field Data: Prior Energy of the Profile, Observation Information Along the Profile Response, and the Non-Close Record Mass hold for the adopted data, its hypothesis (CL) holding with the tolerances εS\varepsilon_{S}, εctl\varepsilon_{\mathrm{ctl}} and the close records Rωcl\mathsf{R}^{\mathrm{cl}}_{\omega} of claim 3 of The Closeness, Fourth-Moment and Discrepancy Hypotheses of the Estimand Assembly Lemma Supplied by an N-Agent Solution under the Cost Bound: Control-Lipschitz Bound on the Record Discrepancy, Close Records from the Path-Closeness Event, and the Explicit Mean-Square Bound; consequently JsymJmf<\mathsf{J}^{\mathrm{sym}}\le\mathsf{J}^{\mathrm{mf}}<\infty, and

NIz=Iu  ((Jmf)1/2+2w1(exp(κmv)1κmv)1/2)2.N\,\mathcal{I}_{\mathsf{z}}=\mathcal{I}_{\mathsf{u}}\ \le\ \Bigl((\mathsf{J}^{\mathrm{mf}})^{1/2}+\sqrt{2}\,\lVert w\rVert_{1}\bigl(\exp(\kappa_{\mathrm{mv}})-1-\kappa_{\mathrm{mv}}\bigr)^{1/2}\Bigr)^{2}.

4. (Pairing of the cell coefficients with the profile response.) For every cLc\in\mathcal{L} and u[0,s]u\in[0,s], Huc2Φˉ2ΛE|H^{c}_{u}|\le\sqrt{2}\,\bar\Phi^{2}\Lambda_{\mathcal{E}}, and for all t,u[0,s]t,u\in[0,s]

ψˉt=[0,t]ΦE(t,u)Θfl(Su,Au)ϖudu,Θfl(Su,Au)ϖu=cLvc(vcϖu)ϕc(u).\bar\psi_{t}=\int_{[0,t]}\Phi^{\mathcal{E}}(t,u')\,\Theta^{\mathrm{fl}}(S_{u'},A_{u'})\,\varpi_{u'}\,du',\qquad \Theta^{\mathrm{fl}}(S_{u},A_{u})\,\varpi_{u}=\sum_{c\in\mathcal{L}}v_{c}\,(v_{c}\cdot\varpi_{u})\,\phi_{c}(u).

Moreover

αz=mNqLwqαq,αzcψˉs  einj,maxqLαaq  2cΦˉ2mN,α  2dcΦˉ2.\alpha\cdot\mathsf{z}=\frac{\mathsf{m}}{N}\sum_{q\in\mathsf{L}}w_{q}\alpha_{q},\qquad \bigl|\alpha\cdot\mathsf{z}-\mathbf{c}\cdot\bar\psi_{s}\bigr|\ \le\ \mathsf{e}_{\mathrm{inj}},\qquad \max_{q\in\mathsf{L}}|\alpha\cdot a_{q}|\ \le\ \frac{\sqrt{2}\,|\mathbf{c}|\,\bar\Phi^{2}\,\mathsf{m}}{\sqrt{N}},\qquad \lVert\alpha\rVert\ \le\ \sqrt{2d}\,|\mathbf{c}|\,\bar\Phi^{2}.
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