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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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· 14,537 chars · 22 deps · depth 20 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 a≥0a\ge0, (1−a)2≥0(1-a)^2\ge0 gives a≤12(1+a2)a\le\tfrac12(1+a^2). Applying this at each ω\omega with a=∣at∣2a=|\mathfrak{a}_t|^2 and a=∣st∣2a=|\mathfrak{s}_t|^2 and taking expectations, hypothesis (M) gives, for every NN and tt,

E[∣at∣2]≤12(1+E[∣at∣4])≤M2,E[∣st∣2]≤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 t↦E[∣at∣2]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 AN≤TM2<∞\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[s0⋅Z0s0]+∫[0,T]E[us⋅Rsus]ds+∫[0,T](2 E[ss⋅Zses]+∑γ,δ=1lZsγδ E[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 s↦E[Θγδ(Σs,αs)]s\mapsto\mathbb{E}[\Theta^{\gamma\delta}(\Sigma_s,\alpha_s)] is bounded and measurable, and by clause (c) there each s↦Θs⋆γδs\mapsto\Theta^{\star\gamma\delta}_s is continuous and bounded; the entries of s↦Zss\mapsto Z_s are continuous and bounded by CZC_Z (conclusion (a) of the completion-of-squares theorem and hypothesis (H2)). Hence s↦∑γδZsγδE[Θγδ(Σs,αs)]s\mapsto\sum_{\gamma\delta}Z^{\gamma\delta}_s\mathbb{E}[\Theta^{\gamma\delta}(\Sigma_s,\alpha_s)] and s↦∑γδZsγδΘs⋆γδs\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 s↦2E[ss⋅Zses]s\mapsto2\mathbb{E}[\mathfrak{s}_s\cdot Z_se_s], the difference of integrable functions, integrable. Subtracting ∫[0,T]∑γδZsγδΘs⋆γδ ds\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]2 E[ss⋅Zses] ds+∫[0,T]∑γ,δ=1lZsγδ(E[Θγδ(Σs,αs)]−Θs⋆γδ)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+6 l K CP\omega_\infty=2K_c+6\,l\,K\,C_P, so that ωL(u)+CP ωb(u)≤ω∞\omega_L(u)+C_P\,\omega_b(u)\le\omega_\infty and ωG(u)≤2Kc\omega_G(u)\le2K_c for every u≥0u\ge0 by conclusion (a) there. Fix δ>0\delta>0. At every point of [0,T]×Ω[0,T]\times\Omega, either ρt≤δ\rho_t\le\delta, and then (ωL(ρt)+CPωb(ρt))(∣st∣2+∣at∣2)≤(ωL(δ)+CPωb(δ))(∣st∣2+∣at∣2)\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 ∣st∣2+∣at∣2=Nρt2>Nδ2|\mathfrak{s}_t|^2+|\mathfrak{a}_t|^2=N\rho_t^2>N\delta^2 and (x+y)2≤2x2+2y2(x+y)^2\le2x^2+2y^2,

(ωL(ρt)+CPωb(ρt))(∣st∣2+∣at∣2)≤ω∞ (∣st∣2+∣at∣2)2Nδ2≤2 ω∞Nδ2(∣st∣4+∣at∣4).\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))(∣st∣2+∣at∣2)]≤2M2(ωL(δ)+CPωb(δ))+4 ω∞MNδ2 ;\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)=N−1/2∣sT∣d(\Sigma_T,S_T)=N^{-1/2}|\mathfrak{s}_T|,

E[ωG(d(ΣT,ST))∣sT∣2]≤ωG(δ) M2+2Kc MNδ2.\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+m2 T(2M2(ωL(δ)+CPωb(δ))+4ω∞MNδ2)+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 N≥N1N\ge N_1; hence ∣RN∣≤ε′′|R_N|\le\varepsilon'' for N≥N1N\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 ∣xγ∣≤∣x∣|x^\gamma|\le|x| of the componentwise calculus toolkit and ∣Zsγδ∣≤CZ|Z^{\gamma\delta}_s|\le C_Z, at every point ∣ss⋅Zses∣≤∑γ,δCZ∣ssγ∣∣esδ∣≤CZ l2 ∣ss∣∣es∣|\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, ∣ss⋅Zses∣≤CZl2ce N−1/2∣ss∣(∣ss∣2+∣as∣2)|\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, (∣s∣−∣s∣2)2≥0(|\mathfrak{s}|-|\mathfrak{s}|^2)^2\ge0 gives ∣s∣3≤12(∣s∣2+∣s∣4)|\mathfrak{s}|^3\le\tfrac12(|\mathfrak{s}|^2+|\mathfrak{s}|^4), and (∣s∣−∣a∣2)2≥0(|\mathfrak{s}|-|\mathfrak{a}|^2)^2\ge0 gives ∣s∣∣a∣2≤12(∣s∣2+∣a∣4)|\mathfrak{s}||\mathfrak{a}|^2\le\tfrac12(|\mathfrak{s}|^2+|\mathfrak{a}|^4); hence with Step 1 and (M), E[∣ss∣(∣ss∣2+∣as∣2)]≤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 ∣2 E[ss⋅Zses]∣≤2 E[∣ss⋅Zses∣]≤2CZl2ceM3N−1/2|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 ±X≤∣X∣\pm X\le|X|), so by monotonicity of the interval integral ∣IIN∣≤2TCZl2ceM3 N−1/2|\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)]−Θs⋆γδ)∣ ≤ CZ l2 cΘN(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 ∣IIIN∣≤TCZl2cΘ(2M2)1/2N−1/2|\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=Rt−1WtT\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 ∣stγ∣≤N|\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[∣at∣2]≤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 Y−X=utY-X=u_t componentwise, and E[ut⋅Rtut]=E[(Y−X)⋅(Rt(Y−X))]\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=stγ−μγ\varepsilon^\gamma_t=\mathfrak{s}^\gamma_t-\mu^\gamma, and conditional expectations μXi\mu_X^i of XiX^i,

E[ut⋅Rtut] ≥ E[εX⋅(RtεX)],εXi=Xi−μXi.\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~,V′U,\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 ∥U−U~∥2=0\lVert U-\tilde{U}\rVert_2=0 by the null-equivalence statement of the square-integrability definition and ∣E[(U−U~)V′]∣≤∥U−U~∥2∥V′∥2=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′=1mRtii′∑γ,δ=1lKiγKi′δ E[εtγεtδ]=∑γ,δ=1l(KTRt K)γδ E[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, Rt−1R_t^{-1} is symmetric positive definite by the invertibility lemma, and

KTRtK=(Rt−1WtT)TRt(Rt−1WtT)=WtRt−1RtRt−1WtT=WtRt−1WtT=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 Rt−1R_t^{-1}. The matrix Ξt\Xi_t is symmetric, ΞtT=Wt(Rt−1)TWtT=Ξt\Xi_t^T=W_t(R_t^{-1})^TW_t^T=\Xi_t, and positive semidefinite: for x∈Rlx\in\mathbb{R}^l, x⋅(Ξtx)=(WtTx)⋅(Rt−1(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 Rt−1R_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[s0⋅Z0s0]=∑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]−Π0γδ∣≤ε′/(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 N≥N1N\ge N_1, whence ∣E[s0⋅Z0s0]−∑γδZ0γδΠ0γδ∣≤l2CZ⋅ε′/(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 ∣rN∣≤ε′/2|r_N|\le\varepsilon'/2 for N≥N2N\ge N_2. For N≥N0=max⁡(N1,N2)N\ge N_0=\max(N_1,N_2), the identity of conclusion (a) gives

JN ≥ ∑γ,δ=1lZ0γδΠ0γδ−ε′2  +  ∫[0,T]E[us(N)⋅Rsus(N)]ds  +  ∫[0,T]∑γ,δ=1lZsγδΘs⋆γδ ds  −  ε′2,\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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