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Proof of Filtering Lower-Bound Reduction of the Recentred N-Agent Cost

lemmalem:n-agent-cost-filtering-reduction-2026a
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Reason: Proof of the filtering lower-bound reduction: uniform second moments from (M), the exact identity from the expansion and completion of squares with delta-splitting and N^{-1/2} error control, the pointwise filtering bound via the conditional mean-square optimality lemma and observation adaptedness, and the epsilon-N assembly.

Proof

Throughout, fix the common data, ZZ, and WW as in the statement, write M2=12(1+M)M_2=\tfrac12(1+M), and abbreviate st=st(N)\mathfrak{s}_t=\mathfrak{s}^{(N)}_t, at=at(N)\mathfrak{a}_t=\mathfrak{a}^{(N)}_t, ut=ut(N)u_t=u^{(N)}_t, Σt=Σt(N)\Sigma_t=\Sigma^{(N)}_t, αt=αt(N)\alpha_t=\alpha^{(N)}_t, and εtγ=εt(N),γ\varepsilon^\gamma_t=\varepsilon^{(N),\gamma}_t when NN is fixed. All pointwise inequalities between random variables below hold at every point of Ω\Omega, and expectations of nonnegative random variables are taken in [0,][0,\infty] with the additivity and monotonicity of the linearity and monotonicity theorem.

Step 1 (second moments and applicability). For a real a0a\ge0, (1a)20(1-a)^2\ge0 gives a12(1+a2)a\le\tfrac12(1+a^2). Applying this at each ω\omega with a=at2a=|\mathfrak{a}_t|^2 and a=st2a=|\mathfrak{s}_t|^2 and taking expectations, hypothesis (M) gives, for every NN and tt,

E[at2]12(1+E[at4])M2,E[st2]M2.\mathbb{E}\big[|\mathfrak{a}_t|^2\big]\le\tfrac12\big(1+\mathbb{E}[|\mathfrak{a}_t|^4]\big)\le M_2,\qquad \mathbb{E}\big[|\mathfrak{s}_t|^2\big]\le M_2 .

The function tE[at2]t\mapsto\mathbb{E}[|\mathfrak{a}_t|^2] is measurable with well-defined Lebesgue integral over the compact interval [0,T][0,T], by part (a) of the a priori second-moment bound, and is bounded by the constant M2M_2, so ANTM2<\mathcal{A}_N\le TM_2<\infty by the monotonicity of the interval integral. Hence the hypothesis of the second-order expansion holds for every NN, and with it all conclusions of the expansion and of the completion-of-squares theorem.

Step 2 (the identity defining rNr_N). Conclusion (c) of the expansion gives JN=LQG[(s),(a)]+RN\mathcal{J}_N=LQG[(\mathfrak{s}),(\mathfrak{a})]+R_N, and conclusion (c) of the completion-of-squares theorem gives

LQG[(s),(a)]=E[s0Z0s0]+[0,T]E[usRsus]ds+[0,T](2E[ssZses]+γ,δ=1lZsγδE[Θγδ(Σs,αs)])ds,LQG[(\mathfrak{s}),(\mathfrak{a})]=\mathbb{E}\big[\mathfrak{s}_0\cdot Z_0\mathfrak{s}_0\big]+\int_{[0,T]}\mathbb{E}\big[u_s\cdot R_su_s\big]ds+\int_{[0,T]}\Big(2\,\mathbb{E}\big[\mathfrak{s}_s\cdot Z_se_s\big]+\sum_{\gamma,\delta=1}^{l}Z^{\gamma\delta}_s\,\mathbb{E}\big[\Theta^{\gamma\delta}(\Sigma_s,\alpha_s)\big]\Big)ds,

with all integrals finite. By clause (b) of the covariance deviation lemma, each sE[Θγδ(Σs,αs)]s\mapsto\mathbb{E}[\Theta^{\gamma\delta}(\Sigma_s,\alpha_s)] is bounded and measurable, and by clause (c) there each sΘsγδs\mapsto\Theta^{\star\gamma\delta}_s is continuous and bounded; the entries of sZss\mapsto Z_s are continuous and bounded by CZC_Z (conclusion (a) of the completion-of-squares theorem and hypothesis (H2)). Hence sγδZsγδE[Θγδ(Σs,αs)]s\mapsto\sum_{\gamma\delta}Z^{\gamma\delta}_s\mathbb{E}[\Theta^{\gamma\delta}(\Sigma_s,\alpha_s)] and sγδZsγδΘsγδs\mapsto\sum_{\gamma\delta}Z^{\gamma\delta}_s\Theta^{\star\gamma\delta}_s are bounded measurable functions with finite interval integrals, so the third integral above splits by the linearity of the interval integral, with s2E[ssZses]s\mapsto2\mathbb{E}[\mathfrak{s}_s\cdot Z_se_s], the difference of integrable functions, integrable. Subtracting [0,T]γδZsγδΘsγδds\int_{[0,T]}\sum_{\gamma\delta}Z^{\gamma\delta}_s\Theta^{\star\gamma\delta}_s\,ds from both sides of the identity of the statement, we conclude that rNr_N is well defined and

rN=RN+[0,T]2E[ssZses]ds+[0,T]γ,δ=1lZsγδ(E[Θγδ(Σs,αs)]Θsγδ)ds  =:  RN+IIN+IIIN.r_N=R_N+\int_{[0,T]}2\,\mathbb{E}\big[\mathfrak{s}_s\cdot Z_se_s\big]\,ds+\int_{[0,T]}\sum_{\gamma,\delta=1}^{l}Z^{\gamma\delta}_s\Big(\mathbb{E}\big[\Theta^{\gamma\delta}(\Sigma_s,\alpha_s)\big]-\Theta^{\star\gamma\delta}_s\Big)ds\;=:\;R_N+\mathrm{II}_N+\mathrm{III}_N .

Step 3 (RNR_N vanishes). Let ωL,ωb,ωG\omega_L,\omega_b,\omega_G and ρt\rho_t be as in the expansion theorem, and set ω=2Kc+6lKCP\omega_\infty=2K_c+6\,l\,K\,C_P, so that ωL(u)+CPωb(u)ω\omega_L(u)+C_P\,\omega_b(u)\le\omega_\infty and ωG(u)2Kc\omega_G(u)\le2K_c for every u0u\ge0 by conclusion (a) there. Fix δ>0\delta>0. At every point of [0,T]×Ω[0,T]\times\Omega, either ρtδ\rho_t\le\delta, and then (ωL(ρt)+CPωb(ρt))(st2+at2)(ωL(δ)+CPωb(δ))(st2+at2)\big(\omega_L(\rho_t)+C_P\omega_b(\rho_t)\big)\big(|\mathfrak{s}_t|^2+|\mathfrak{a}_t|^2\big)\le\big(\omega_L(\delta)+C_P\omega_b(\delta)\big)\big(|\mathfrak{s}_t|^2+|\mathfrak{a}_t|^2\big) since the moduli are nondecreasing, or ρt>δ\rho_t>\delta, and then, because st2+at2=Nρt2>Nδ2|\mathfrak{s}_t|^2+|\mathfrak{a}_t|^2=N\rho_t^2>N\delta^2 and (x+y)22x2+2y2(x+y)^2\le2x^2+2y^2,

(ωL(ρt)+CPωb(ρt))(st2+at2)ω(st2+at2)2Nδ22ωNδ2(st4+at4).\big(\omega_L(\rho_t)+C_P\omega_b(\rho_t)\big)\big(|\mathfrak{s}_t|^2+|\mathfrak{a}_t|^2\big)\le\omega_\infty\,\frac{\big(|\mathfrak{s}_t|^2+|\mathfrak{a}_t|^2\big)^2}{N\delta^2}\le\frac{2\,\omega_\infty}{N\delta^2}\big(|\mathfrak{s}_t|^4+|\mathfrak{a}_t|^4\big).

Adding the two bounds and taking expectations, using Step 1 and (M),

E[(ωL(ρt)+CPωb(ρt))(st2+at2)]2M2(ωL(δ)+CPωb(δ))+4ωMNδ2;\mathbb{E}\Big[\big(\omega_L(\rho_t)+C_P\omega_b(\rho_t)\big)\big(|\mathfrak{s}_t|^2+|\mathfrak{a}_t|^2\big)\Big]\le2M_2\big(\omega_L(\delta)+C_P\omega_b(\delta)\big)+\frac{4\,\omega_\infty M}{N\delta^2}\,;

the integral over [0,T][0,T] of the left-hand side is well defined and finite by conclusion (b) of the expansion, and is at most TT times the constant right-hand side by monotonicity. Similarly, since d(ΣT,ST)=N1/2sTd(\Sigma_T,S_T)=N^{-1/2}|\mathfrak{s}_T|,

E[ωG(d(ΣT,ST))sT2]ωG(δ)M2+2KcMNδ2.\mathbb{E}\Big[\omega_G\big(d(\Sigma_T,S_T)\big)|\mathfrak{s}_T|^2\Big]\le\omega_G(\delta)\,M_2+\frac{2K_c\,M}{N\delta^2}.

By conclusion (c) of the expansion,

RN  l+m2T(2M2(ωL(δ)+CPωb(δ))+4ωMNδ2)+l2(ωG(δ)M2+2KcMNδ2).|R_N|\ \le\ \frac{l+m}{2}\,T\Big(2M_2\big(\omega_L(\delta)+C_P\omega_b(\delta)\big)+\frac{4\omega_\infty M}{N\delta^2}\Big)+\frac{l}{2}\Big(\omega_G(\delta)M_2+\frac{2K_cM}{N\delta^2}\Big).

Given ε>0\varepsilon''>0, conclusion (a) of the expansion provides δ>0\delta>0 with ωL(δ)+CPωb(δ)\omega_L(\delta)+C_P\omega_b(\delta) and ωG(δ)\omega_G(\delta) so small that the δ\delta-terms sum to at most ε/2\varepsilon''/2, and then N1N_1 with the 1/N1/N-terms at most ε/2\varepsilon''/2 for NN1N\ge N_1; hence RNε|R_N|\le\varepsilon'' for NN1N\ge N_1, and (RN)(R_N) has limit 00.

Step 4 (IIN\mathrm{II}_N and IIIN\mathrm{III}_N vanish). By the componentwise estimate xγx|x^\gamma|\le|x| of the componentwise calculus toolkit and ZsγδCZ|Z^{\gamma\delta}_s|\le C_Z, at every point ssZsesγ,δCZssγesδCZl2sses|\mathfrak{s}_s\cdot Z_se_s|\le\sum_{\gamma,\delta}C_Z|\mathfrak{s}^\gamma_s||e^\delta_s|\le C_Z\,l^2\,|\mathfrak{s}_s||e_s|, so by conclusion (b) of the completion-of-squares theorem, ssZsesCZl2ceN1/2ss(ss2+as2)|\mathfrak{s}_s\cdot Z_se_s|\le C_Zl^2c_e\,N^{-1/2}|\mathfrak{s}_s|\big(|\mathfrak{s}_s|^2+|\mathfrak{a}_s|^2\big). Pointwise, (ss2)20(|\mathfrak{s}|-|\mathfrak{s}|^2)^2\ge0 gives s312(s2+s4)|\mathfrak{s}|^3\le\tfrac12(|\mathfrak{s}|^2+|\mathfrak{s}|^4), and (sa2)20(|\mathfrak{s}|-|\mathfrak{a}|^2)^2\ge0 gives sa212(s2+a4)|\mathfrak{s}||\mathfrak{a}|^2\le\tfrac12(|\mathfrak{s}|^2+|\mathfrak{a}|^4); hence with Step 1 and (M), E[ss(ss2+as2)]M2+M=:M3\mathbb{E}\big[|\mathfrak{s}_s|(|\mathfrak{s}_s|^2+|\mathfrak{a}_s|^2)\big]\le M_2+M=:M_3 for every ss. Therefore 2E[ssZses]2E[ssZses]2CZl2ceM3N1/2|2\,\mathbb{E}[\mathfrak{s}_s\cdot Z_se_s]|\le2\,\mathbb{E}\big[|\mathfrak{s}_s\cdot Z_se_s|\big]\le2C_Zl^2c_eM_3N^{-1/2} for every ss (monotonicity, and ±XX\pm X\le|X|), so by monotonicity of the interval integral IIN2TCZl2ceM3N1/2|\mathrm{II}_N|\le2TC_Zl^2c_eM_3\,N^{-1/2}, and (IIN)(\mathrm{II}_N) has limit 00. For IIIN\mathrm{III}_N: with cΘc_\Theta as in the covariance deviation lemma, its clause (b) and Step 1 give, for every ss,

γ,δ=1lZsγδ(E[Θγδ(Σs,αs)]Θsγδ)  CZl2cΘN(2M2)1/2,\Big|\sum_{\gamma,\delta=1}^{l}Z^{\gamma\delta}_s\Big(\mathbb{E}\big[\Theta^{\gamma\delta}(\Sigma_s,\alpha_s)\big]-\Theta^{\star\gamma\delta}_s\Big)\Big|\ \le\ C_Z\,l^2\,\frac{c_\Theta}{\sqrt{N}}\big(2M_2\big)^{1/2},

so IIINTCZl2cΘ(2M2)1/2N1/2|\mathrm{III}_N|\le TC_Zl^2c_\Theta(2M_2)^{1/2}N^{-1/2}, and (IIIN)(\mathrm{III}_N) has limit 00. Combining Steps 3--4 with the triangle inequality, (rN)(r_N) has limit 00. Together with the finiteness assertions of Step 2 this proves conclusion (a).

Step 5 (filtering bound). Fix NN and tt, and write K=Rt1WtT\mathcal{K}=R_t^{-1}W_t^T, a real matrix with mm rows and ll columns with entries bounded by CKC_K (conclusion (a) of the completion-of-squares theorem). Each component of st\mathfrak{s}_t is bounded: every coordinate of the empirical state measure and of StS_t lies in [0,1][0,1], both lying in the probability simplex at every ω\omega, so stγN|\mathfrak{s}^\gamma_t|\le\sqrt{N} at every ω\omega, and bounded random variables are square-integrable by monotonicity. Each component of at\mathfrak{a}_t satisfies E[(atj)2]E[at2]M2\mathbb{E}[(\mathfrak{a}^j_t)^2]\le\mathbb{E}[|\mathfrak{a}_t|^2]\le M_2 (componentwise estimate and Step 1), hence is square-integrable, and is almost surely equal to a Gt(N)\mathcal{G}^{(N)}_t-measurable square-integrable random variable by conclusions 2--3 of the observation-adaptedness lemma. Set X=KstX=-\mathcal{K}\mathfrak{s}_t componentwise, so Xi=γ=1lKiγstγX^i=-\sum_{\gamma=1}^{l}\mathcal{K}^{i\gamma}\mathfrak{s}^\gamma_t is square-integrable by the closure properties of the square-integrability definition, and Y=atY=\mathfrak{a}_t; then YX=utY-X=u_t componentwise, and E[utRtut]=E[(YX)(Rt(YX))]\mathbb{E}[u_t\cdot R_tu_t]=\mathbb{E}[(Y-X)\cdot(R_t(Y-X))], the entry pairing of the completion-of-squares theorem and the index formula of the conditional mean-square optimality lemma being the identical double sum. Each RtR_t is symmetric positive definite (conclusion (a) of the completion-of-squares theorem), hence positive semidefinite, so that lemma applies with k=mk=m, G=Gt(N)\mathcal{G}=\mathcal{G}^{(N)}_t, and weight RtR_t: fixing conditional expectations μγ\mu^\gamma of stγ\mathfrak{s}^\gamma_t given Gt(N)\mathcal{G}^{(N)}_t, so that εtγ=stγμγ\varepsilon^\gamma_t=\mathfrak{s}^\gamma_t-\mu^\gamma, and conditional expectations μXi\mu_X^i of XiX^i,

E[utRtut]  E[εX(RtεX)],εXi=XiμXi.\mathbb{E}\big[u_t\cdot R_tu_t\big]\ \ge\ \mathbb{E}\big[\varepsilon_X\cdot(R_t\varepsilon_X)\big],\qquad \varepsilon_X^i=X^i-\mu_X^i .

By the linearity of conditional expectation (part 1 of the basic properties lemma, applied finitely many times), γKiγμγ-\sum_\gamma\mathcal{K}^{i\gamma}\mu^\gamma is a conditional expectation of XiX^i, so μXi=γKiγμγ\mu_X^i=-\sum_\gamma\mathcal{K}^{i\gamma}\mu^\gamma almost surely by the uniqueness assertion of the existence and uniqueness theorem; hence εXi=γKiγεtγ\varepsilon_X^i=-\sum_\gamma\mathcal{K}^{i\gamma}\varepsilon^\gamma_t almost surely. For square-integrable U,U~,VU,\tilde{U},V' with UU almost surely equal to U~\tilde{U} one has E[UV]=E[U~V]\mathbb{E}[UV']=\mathbb{E}[\tilde{U}V'], since UU~2=0\lVert U-\tilde{U}\rVert_2=0 by the null-equivalence statement of the square-integrability definition and E[(UU~)V]UU~2V2=0|\mathbb{E}[(U-\tilde{U})V']|\le\lVert U-\tilde{U}\rVert_2\lVert V'\rVert_2=0 by the Cauchy--Schwarz inequality; a product both of whose factors are replaced by almost-sure equals requires two applications, one factor at a time. Applying this and the linearity of the integral entrywise,

E[εX(RtεX)]=i,i=1mRtiiγ,δ=1lKiγKiδE[εtγεtδ]=γ,δ=1l(KTRtK)γδE[εtγεtδ],\mathbb{E}\big[\varepsilon_X\cdot(R_t\varepsilon_X)\big]=\sum_{i,i'=1}^{m}R^{ii'}_t\sum_{\gamma,\delta=1}^{l}\mathcal{K}^{i\gamma}\mathcal{K}^{i'\delta}\,\mathbb{E}\big[\varepsilon^\gamma_t\varepsilon^\delta_t\big]=\sum_{\gamma,\delta=1}^{l}\big(\mathcal{K}^T R_t\,\mathcal{K}\big)^{\gamma\delta}\,\mathbb{E}\big[\varepsilon^\gamma_t\varepsilon^\delta_t\big],

by the entry formulas for matrix products and the transpose. Since RtR_t is symmetric positive definite, Rt1R_t^{-1} is symmetric positive definite by the invertibility lemma, and

KTRtK=(Rt1WtT)TRt(Rt1WtT)=WtRt1RtRt1WtT=WtRt1WtT=Ξt,\mathcal{K}^TR_t\mathcal{K}=(R_t^{-1}W_t^T)^TR_t(R_t^{-1}W_t^T)=W_tR_t^{-1}R_tR_t^{-1}W_t^T=W_tR_t^{-1}W_t^T=\Xi_t,

using the identity (UV)T=VTUT(UV)^T=V^TU^T of claim 3 of the componentwise calculus toolkit, the involutivity (MT)T=M(M^T)^T=M, immediate from the definition of the transpose, and the symmetry of Rt1R_t^{-1}. The matrix Ξt\Xi_t is symmetric, ΞtT=Wt(Rt1)TWtT=Ξt\Xi_t^T=W_t(R_t^{-1})^TW_t^T=\Xi_t, and positive semidefinite: for xRlx\in\mathbb{R}^l, x(Ξtx)=(WtTx)(Rt1(WtTx))0x\cdot(\Xi_tx)=(W_t^Tx)\cdot\big(R_t^{-1}(W_t^Tx)\big)\ge0, using the identity y(Mz)=(MTy)zy\cdot(Mz)=(M^Ty)\cdot z of claim 3 of the toolkit and the positive definiteness of Rt1R_t^{-1}. Finally γδΞtγδE[εtγεtδ]=E[εt(Ξtεt)]0\sum_{\gamma\delta}\Xi^{\gamma\delta}_t\mathbb{E}[\varepsilon^\gamma_t\varepsilon^\delta_t]=\mathbb{E}[\varepsilon_t\cdot(\Xi_t\varepsilon_t)]\ge0 by claim 1 of the expected quadratic form lemma and the pointwise nonnegativity of εt(ω)(Ξtεt(ω))\varepsilon_t(\omega)\cdot(\Xi_t\varepsilon_t(\omega)) with monotonicity of the integral. If μˉγ\bar{\mu}^\gamma is another choice of conditional expectations, each μˉγ\bar{\mu}^\gamma is almost surely equal to μγ\mu^\gamma by the uniqueness assertion, so each product expectation E[εtγεtδ]\mathbb{E}[\varepsilon^\gamma_t\varepsilon^\delta_t] is unchanged, again by two applications of the almost-sure substitution above; the middle quantity is therefore independent of the choice. This proves conclusion (b).

Step 6 (lower bound). By claim 1 of the expected quadratic form lemma, E[s0Z0s0]=γδZ0γδE[s0γs0δ]\mathbb{E}[\mathfrak{s}_0\cdot Z_0\mathfrak{s}_0]=\sum_{\gamma\delta}Z_0^{\gamma\delta}\mathbb{E}[\mathfrak{s}_0^\gamma\mathfrak{s}_0^\delta]. Let ε>0\varepsilon'>0. By hypothesis (I) there is N1N_1 such that E[s0(N),γs0(N),δ]Π0γδε/(2l2CZ+2)|\mathbb{E}[\mathfrak{s}^{(N),\gamma}_0\mathfrak{s}^{(N),\delta}_0]-\Pi_0^{\gamma\delta}|\le\varepsilon'/(2l^2C_Z+2) for all γ,δ\gamma,\delta and NN1N\ge N_1, whence E[s0Z0s0]γδZ0γδΠ0γδl2CZε/(2l2CZ+2)ε/2\big|\mathbb{E}[\mathfrak{s}_0\cdot Z_0\mathfrak{s}_0]-\sum_{\gamma\delta}Z_0^{\gamma\delta}\Pi_0^{\gamma\delta}\big|\le l^2C_Z\cdot\varepsilon'/(2l^2C_Z+2)\le\varepsilon'/2; and by conclusion (a) there is N2N_2 with rNε/2|r_N|\le\varepsilon'/2 for NN2N\ge N_2. For NN0=max(N1,N2)N\ge N_0=\max(N_1,N_2), the identity of conclusion (a) gives

JN  γ,δ=1lZ0γδΠ0γδε2  +  [0,T]E[us(N)Rsus(N)]ds  +  [0,T]γ,δ=1lZsγδΘsγδds    ε2,\mathcal{J}_N\ \ge\ \sum_{\gamma,\delta=1}^{l}Z^{\gamma\delta}_0\Pi^{\gamma\delta}_0-\tfrac{\varepsilon'}{2}\;+\;\int_{[0,T]}\mathbb{E}\big[u^{(N)}_s\cdot R_su^{(N)}_s\big]ds\;+\;\int_{[0,T]}\sum_{\gamma,\delta=1}^{l}Z^{\gamma\delta}_s\Theta^{\star\gamma\delta}_s\,ds\;-\;\tfrac{\varepsilon'}{2},

which is conclusion (c). \square

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