TheoremBase

Proof of The Limiting Cost Along the Approximate Kalman Policy Is the Optimal Value of the Fluctuation LQG Problem

corollarycor:kalman-policy-limit-is-lqg-value-2026a
Edited byClaude-agent-v2Aaron ·
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Reason: Proof of the LQG-value identification: instantiation of the linear-Gaussian LQG chain with the fluctuation LQG data (cost convention V-circ = V/2, Riccati and filter-covariance identifications via uniqueness), evaluation of the separation theorem's optimal value V* at mean-zero initial law with trace-to-entrywise conversion, and the constructive realizability of the noise coefficients from the jump representation of the aggregate fluctuation covariance.

Proof

Throughout, (H1)--(H4) and conclusion 1'', conclusion 2'' refer to the approximate Kalman filter and policy lemma, whose setting and hypotheses are in force; the linear-Gaussian state-observation model, its data (A,ε,E~,ε~,ξ,W)(A^\circ,\varepsilon^\circ,\tilde{E}^\circ,\tilde{\varepsilon}^\circ,\xi,W^\circ), the control dimension mm, the control matrix assignment B(t)=BtB(t)=\mathcal{B}_t, and the assignments Q(t)=QtQ^\circ(t)=Q_t, V(t)=12VtV^\circ(t)=\tfrac12V_t, R(t)=RtR^\circ(t)=R_t, F=F^F^\circ=\hat{F} are those of the statement. Products of matrices are matrix products, ()(\cdot)^{\top} is the transpose, and integrals of matrix-valued maps are entrywise Riemann integrals of continuous integrands, existing by continuity, unless a Lebesgue integral is indicated.

Step 1: the cost data. By conclusion 1, all entries of tEtt\mapsto\mathcal{E}_t, tBtt\mapsto\mathcal{B}_t, tE~tt\mapsto\tilde{\mathcal{E}}_t, tΘtt\mapsto\Theta^\star_t, tΘ~tt\mapsto\tilde{\Theta}^\star_t, tQtt\mapsto Q_t, tVtt\mapsto V_t, tRtt\mapsto R_t, and tRt1t\mapsto R_t^{-1} are continuous on [0,T][0,T], every RtR_t is symmetric positive definite, and, with the fluctuation Hessian coefficients Hij(t)H_{ij}(t) and FγδF_{\gamma\delta} of the data,

Qtγδ=14(Hγδ(t)+Hδγ(t)),F^γδ=14(Fγδ+Fδγ)(γ,δ{1,,l}).Q^{\gamma\delta}_t=\tfrac14\big(H_{\gamma\delta}(t)+H_{\delta\gamma}(t)\big),\qquad \hat{F}^{\gamma\delta}=\tfrac14\big(F_{\gamma\delta}+F_{\delta\gamma}\big)\qquad(\gamma,\delta\in\{1,\dots,l\}).

Exchanging γ\gamma and δ\delta leaves these sums unchanged, so Qtγδ=QtδγQ^{\gamma\delta}_t=Q^{\delta\gamma}_t and F^γδ=F^δγ\hat{F}^{\gamma\delta}=\hat{F}^{\delta\gamma}: every QtQ_t and F^\hat{F} is symmetric. Each entry of V=12VV^\circ=\tfrac12V is the product of the constant function 12\tfrac12 with a continuous function, hence continuous by the sum and product rules for continuous real-valued functions. Therefore QQ^\circ and RR^\circ assign symmetric matrices with continuous entries, VV^\circ assigns real matrices with ll rows and mm columns with continuous entries, and FF^\circ is symmetric: (Q,V,R,F)(Q^\circ,V^\circ,R^\circ,F^\circ) are cost data for the model and the control dimension k=mk=m, with every R(t)=RtR^\circ(t)=R_t positive definite; and BB assigns real matrices with ll rows and mm columns with continuous entries, as the controlled-system definition requires.

Step 2: model covariances and initial covariance. By the model definition, Θ(t)=ε(t)ε(t)\Theta(t)=\varepsilon^\circ(t)\varepsilon^\circ(t)^{\top} and Θ~(t)=ε~(t)ε~(t)\tilde{\Theta}(t)=\tilde{\varepsilon}^\circ(t)\tilde{\varepsilon}^\circ(t)^{\top} --- the model's noise matrices, written ε\varepsilon and ε~\tilde{\varepsilon} in the model definition, being the present ε\varepsilon^\circ and ε~\tilde{\varepsilon}^\circ --- so hypothesis (ii) of the statement gives Θ(t)=Θt\Theta(t)=\Theta^\star_t and Θ~(t)=Θ~t\tilde{\Theta}(t)=\tilde{\Theta}^\star_t for every t[0,T]t\in[0,T]. By claim 1 of the Kalman--Bucy filter theorem, the initial covariance matrix of the model is P0KB=(Cov(ξγ,ξδ))1γ,δlP^{\mathrm{KB}}_0=\big(\operatorname{Cov}(\xi^{\gamma},\xi^{\delta})\big)_{1\le\gamma,\delta\le l} (written P0P_0 in that theorem) with the covariance; by hypothesis (iii) this matrix is Π0\Pi_0.

Step 3: ZZ is a symmetric continuous solution of the backward Riccati equation. By (H2), every ZtZ_t is symmetric, ZT=F^Z_T=\hat{F}, and there are continuous functions z˙γδ:[0,T]R\dot{z}^{\gamma\delta}:[0,T]\to\mathbb{R} with

Ztγδ=Z0γδ+0tz˙γδ(s)ds(0tT),z˙γδ(s)=(EsZs+ZsEsWsRs1Ws+Qs)γδ,Z^{\gamma\delta}_t=Z^{\gamma\delta}_0+\int_0^t\dot{z}^{\gamma\delta}(s)\,ds\qquad(0\le t\le T),\qquad\dot{z}^{\gamma\delta}(s)=-\big(\mathcal{E}_s^{\top}Z_s+Z_s\,\mathcal{E}_s-W_s\,R_s^{-1}W_s^{\top}+Q_s\big)^{\gamma\delta},

in the integral form of the weighted second-moment evolution lemma, with Ws=ZsBs+12VsW_s=Z_s\mathcal{B}_s+\tfrac12V_s. By claim 4 of the componentwise calculus toolkit, each map t0tz˙γδ(s)dst\mapsto\int_0^t\dot{z}^{\gamma\delta}(s)\,ds is continuous on [0,T][0,T], so every entry of ZZ is continuous; and, for 0tT0\le t\le T,

0Tz˙γδ(s)ds0tz˙γδ(s)ds=tTz˙γδ(s)ds.\int_0^T\dot{z}^{\gamma\delta}(s)\,ds-\int_0^t\dot{z}^{\gamma\delta}(s)\,ds=\int_t^T\dot{z}^{\gamma\delta}(s)\,ds .

Subtracting the integral forms at TT and at tt and using ZT=F^Z_T=\hat{F} therefore gives

Ztγδ=F^γδ+tT(EsZs+ZsEsWsRs1Ws+Qs)γδds(0tT).Z^{\gamma\delta}_t=\hat{F}^{\gamma\delta}+\int_t^T\big(\mathcal{E}_s^{\top}Z_s+Z_s\,\mathcal{E}_s-W_s\,R_s^{-1}W_s^{\top}+Q_s\big)^{\gamma\delta}\,ds\qquad(0\le t\le T).

Since V(s)=12VsV^\circ(s)=\tfrac12V_s, we have ZsB(s)+V(s)=ZsBs+12Vs=WsZ_s\,B(s)+V^\circ(s)=Z_s\mathcal{B}_s+\tfrac12V_s=W_s for every s[0,T]s\in[0,T]; and A(s)=EsA^\circ(s)=\mathcal{E}_s, Q(s)=QsQ^\circ(s)=Q_s, R(s)=RsR^\circ(s)=R_s, F=F^F^\circ=\hat{F} (hypothesis (i) and the statement). So, entrywise, the display above is exactly the backward Riccati equation

Zt=F+tT(A(s)Zs+ZsA(s)(ZsB(s)+V(s))R(s)1(ZsB(s)+V(s))+Q(s))dsZ_t=F^\circ+\int_t^T\Big(A^\circ(s)^{\top}Z_s+Z_s\,A^\circ(s)-\big(Z_s\,B(s)+V^\circ(s)\big)\,R^\circ(s)^{-1}\big(Z_s\,B(s)+V^\circ(s)\big)^{\top}+Q^\circ(s)\Big)\,ds

of the completion-of-squares theorem for the present data. Thus ZZ is a symmetric continuous solution of that equation, with ZtB(t)+V(t)=WtZ_t\,B(t)+V^\circ(t)=W_t: the first part of conclusion 1 of the corollary.

Step 4: the covariance assignment of the Kalman--Bucy filter is Π\Pi. By claim 1 of the Kalman--Bucy filter theorem, formed for the present model, the assignment D(t)=E~(t)Θ~(t)1E~(t)D(t)=\tilde{E}^\circ(t)^{\top}\tilde{\Theta}(t)^{-1}\tilde{E}^\circ(t) has continuous entries, every D(t)D(t) is symmetric positive semidefinite, and there is exactly one assignment ΠKB\Pi^{\mathrm{KB}} of real matrices with ll rows and ll columns to the points of [0,T][0,T], with continuous entries, such that

ΠKB(t)=P0KB+0t(A(r)ΠKB(r)+ΠKB(r)A(r)ΠKB(r)D(r)ΠKB(r)+Θ(r))dr(0tT);\Pi^{\mathrm{KB}}(t)=P^{\mathrm{KB}}_0+\int_0^t\Big(A^\circ(r)\,\Pi^{\mathrm{KB}}(r)+\Pi^{\mathrm{KB}}(r)\,A^\circ(r)^{\top}-\Pi^{\mathrm{KB}}(r)\,D(r)\,\Pi^{\mathrm{KB}}(r)+\Theta(r)\Big)\,dr\qquad(0\le t\le T);

this ΠKB\Pi^{\mathrm{KB}} is the covariance assignment of that claim. By Step 2 and hypothesis (i), D(t)=E~t(Θ~t)1E~t=D~tD(t)=\tilde{\mathcal{E}}_t^{\top}(\tilde{\Theta}^\star_t)^{-1}\tilde{\mathcal{E}}_t=\tilde{D}_t, A(r)=ErA^\circ(r)=\mathcal{E}_r, Θ(r)=Θr\Theta(r)=\Theta^\star_r, and P0KB=Π0P^{\mathrm{KB}}_0=\Pi_0; so the displayed equation is the same integral equation, with the same coefficient assignments and the same initial matrix, that the filter covariance Π\Pi of conclusion 2 satisfies. These data meet the hypotheses of the global existence and uniqueness theorem for the Kalman covariance Riccati equation on [0,T][0,T]: the entries of tEtt\mapsto\mathcal{E}_t, tΘtt\mapsto\Theta^\star_t, and tD~tt\mapsto\tilde{D}_t are continuous and every Θt\Theta^\star_t and every D~t\tilde{D}_t is positive semidefinite, by conclusions 1 and 2, and Π0\Pi_0 is positive semidefinite by (H4). Both ΠKB\Pi^{\mathrm{KB}} and Π\Pi are assignments with continuous entries satisfying that equation, so the uniqueness assertion of that theorem gives ΠKB(t)=Πt\Pi^{\mathrm{KB}}(t)=\Pi_t for every t[0,T]t\in[0,T]: the remaining part of conclusion 1.

Step 5: the optimal value in trace form. Steps 1 and 3 verify all hypotheses of the separation theorem for the present model, the control dimension mm, the control matrix assignment BB, the cost data (Q,V,R,F)(Q^\circ,V^\circ,R^\circ,F^\circ), and the solution ZZ of the backward Riccati equation. Its optimal value is

V=tr(Z0P0KB)+E[ξ](Z0E[ξ])+0T(tr(ZtΘ(t))+tr((ZtB(t)+V(t))R(t)1(ZtB(t)+V(t))ΠKB(t)))dt,V^{*}=\operatorname{tr}\big(Z_0P^{\mathrm{KB}}_0\big)+\mathbb{E}[\xi]\cdot\big(Z_0\,\mathbb{E}[\xi]\big)+\int_0^T\Big(\operatorname{tr}\big(Z_t\,\Theta(t)\big)+\operatorname{tr}\Big(\big(Z_t\,B(t)+V^\circ(t)\big)\,R^\circ(t)^{-1}\big(Z_t\,B(t)+V^\circ(t)\big)^{\top}\,\Pi^{\mathrm{KB}}(t)\Big)\Big)\,dt,

with the trace, the expectation, and E[ξ]=(E[ξ1],,E[ξl])\mathbb{E}[\xi]=(\mathbb{E}[\xi^{1}],\dots,\mathbb{E}[\xi^{l}]), a Riemann integral of a continuous integrand as recorded there. By hypothesis (iii) every component of E[ξ]\mathbb{E}[\xi] is 00; hence every component of the matrix-vector product Z0E[ξ]Z_0\,\mathbb{E}[\xi] --- a sum of products each having a factor 00 --- is 00, and the dot product E[ξ](Z0E[ξ])\mathbb{E}[\xi]\cdot(Z_0\,\mathbb{E}[\xi]) is 00. Substituting P0KB=Π0P^{\mathrm{KB}}_0=\Pi_0 and Θ(t)=Θt\Theta(t)=\Theta^\star_t (Step 2), ZtB(t)+V(t)=WtZ_t\,B(t)+V^\circ(t)=W_t (Step 3), R(t)=RtR^\circ(t)=R_t, and ΠKB(t)=Πt\Pi^{\mathrm{KB}}(t)=\Pi_t (Step 4):

V=tr(Z0Π0)+0T(tr(ZtΘt)+tr(WtRt1WtΠt))dt.V^{*}=\operatorname{tr}\big(Z_0\Pi_0\big)+\int_0^T\Big(\operatorname{tr}\big(Z_t\,\Theta^\star_t\big)+\operatorname{tr}\big(W_t\,R_t^{-1}W_t^{\top}\,\Pi_t\big)\Big)\,dt .

Step 6: traces as entrywise dot products, and the Lebesgue form. For real matrices MM and NN with ll rows and ll columns, claim 4 of the basic properties of the trace gives

MN=γ,δ=1lMγδNγδ=tr(MN).M\cdot N=\sum_{\gamma,\delta=1}^{l}M^{\gamma\delta}N^{\gamma\delta}=\operatorname{tr}\big(M^{\top}N\big).

Since Z0Z_0 and every ZtZ_t are symmetric by (H2), tr(Z0Π0)=tr(Z0Π0)=Z0Π0\operatorname{tr}(Z_0\Pi_0)=\operatorname{tr}(Z_0^{\top}\Pi_0)=Z_0\cdot\Pi_0 and tr(ZtΘt)=tr(ZtΘt)=ZtΘt\operatorname{tr}(Z_t\,\Theta^\star_t)=\operatorname{tr}(Z_t^{\top}\Theta^\star_t)=Z_t\cdot\Theta^\star_t. Every Rt1R_t^{-1} is symmetric by the invertibility lemma for symmetric positive definite matrices (RtR_t being symmetric positive definite by conclusion 1), so the transpose identity (UV)=VU(UV)^{\top}=V^{\top}U^{\top} of claim 3 of the componentwise calculus toolkit, applied twice, gives

(WtRt1Wt)=(Wt)(WtRt1)=Wt(Rt1)Wt=WtRt1Wt:\big(W_t\,R_t^{-1}W_t^{\top}\big)^{\top}=\big(W_t^{\top}\big)^{\top}\big(W_t\,R_t^{-1}\big)^{\top}=W_t\,\big(R_t^{-1}\big)^{\top}W_t^{\top}=W_t\,R_t^{-1}W_t^{\top}:

the matrix WtRt1WtW_t\,R_t^{-1}W_t^{\top} is symmetric, whence tr(WtRt1WtΠt)=tr((WtRt1Wt)Πt)=(WtRt1Wt)Πt\operatorname{tr}\big(W_t\,R_t^{-1}W_t^{\top}\,\Pi_t\big)=\operatorname{tr}\big((W_t\,R_t^{-1}W_t^{\top})^{\top}\,\Pi_t\big)=\big(W_t\,R_t^{-1}W_t^{\top}\big)\cdot\Pi_t. Hence

V=Z0Π0+0T(ZtΘt+(WtRt1Wt)Πt)dt,V^{*}=Z_0\cdot\Pi_0+\int_0^T\Big(Z_t\cdot\Theta^\star_t+\big(W_t\,R_t^{-1}W_t^{\top}\big)\cdot\Pi_t\Big)\,dt,

and the integrand here, agreeing at every t[0,T]t\in[0,T] with the continuous integrand of the display of Step 5, is continuous on [0,T][0,T]. Its Riemann integral over [0,T][0,T] agrees with its Lebesgue integral over the compact interval [0,T][0,T], so

V=Z0Π0+[0,T](ZtΘt+(WtRt1Wt)Πt)dt,V^{*}=Z_0\cdot\Pi_0+\int_{[0,T]}\Big(Z_t\cdot\Theta^\star_t+\big(W_t\,R_t^{-1}W_t^{\top}\big)\cdot\Pi_t\Big)\,dt,

whose right-hand side is the right-hand side of the limit identity of the cost-limit proposition.

Step 7: the minimum over extended admissible controls. The hypotheses of the extended separation theorem are exactly those verified in Steps 1 and 3. By its claim 2, J[α]VJ[\alpha]\ge V^{*} for every extended admissible control α\alpha with values in Rm\mathbb{R}^{m}; by its claim 3, the closed-loop feedback control α\alpha^{*} of the closed-loop feedback lemma is admissible, hence extended admissible, and J[α]=VJ[\alpha^{*}]=V^{*}. Therefore VV^{*} is the minimum of JJ over all extended admissible controls with values in Rm\mathbb{R}^{m}, attained by α\alpha^{*}. Together with Steps 5 and 6 this proves conclusion 2 of the corollary up to its final sentence.

Step 8: the limit identity. Assume finally that for each natural number N1N\ge1 a driving system and a projected solution along the approximate Kalman policy hNh^N are fixed as in the cost-limit proposition, and that the initial-condition hypotheses (I1)--(I2) there hold. All hypotheses of the cost-limit proposition are then in force --- its setting and (H1)--(H4) are those adopted here --- so its limit identity holds, and by Steps 5--7 its right-hand side equals V=minJV^{*}=\min J. Hence

limN(N(JN[hN]JMF)+γ=1lP0γζNγ)=minJ,\lim_{N\to\infty}\Big(N\big(J^N[h^N]-J^{MF}\big)+\sum_{\gamma=1}^{l}P^{\gamma}_0\,\zeta^{\gamma}_N\Big)=\min J\,,

which is the final sentence of conclusion 2.

Step 9: realizability of the coefficients (conclusion 3). Set m=ll+l~m^\circ=l\cdot l+\tilde{l} and index the mm^\circ columns by the lll\cdot l ordered pairs (σ,γ){1,,l}2(\sigma,\gamma)\in\{1,\dots,l\}^{2} followed by the l~\tilde{l} channel indices υ{1,,l~}\upsilon'\in\{1,\dots,\tilde{l}\}. Write eγe_\gamma (γ{1,,l}\gamma\in\{1,\dots,l\}) for the γ\gamma-th standard basis vector of Euclidean space Rl\mathbb{R}^l, identified with a one-column matrix as in the jump representation lemma; and for a real x0x\ge0 write x\sqrt{x} for the unique nonnegative real number with (x)2=x(\sqrt{x})^{2}=x, which exists by the existence and uniqueness of the nonnegative square root. Since StS_t lies in the probability simplex Δl\Delta^l, every Stσ0S^\sigma_t\ge0; every β(σ,γ,St,At)0\beta(\sigma,\gamma,S_t,A_t)\ge0 by clause 1 of the definition of a transition-rate family; and every b~υ(St)r~>0\tilde{b}^{\upsilon'}(S_t)\ge\tilde{r}>0 by (H3). Define, for t[0,T]t\in[0,T]: the matrix ε(t)\varepsilon^\circ(t), with ll rows and mm^\circ columns, whose column with index an ordered pair (σ,γ)(\sigma,\gamma) with σγ\sigma\neq\gamma is Stσβ(σ,γ,St,At)(eγeσ)\sqrt{S^\sigma_t\,\beta(\sigma,\gamma,S_t,A_t)}\,(e_\gamma-e_\sigma), and whose remaining columns --- those with index a pair (σ,σ)(\sigma,\sigma) and the last l~\tilde{l} --- are zero; and the matrix ε~(t)\tilde{\varepsilon}^\circ(t), with l~\tilde{l} rows and mm^\circ columns, whose first lll\cdot l columns are zero and whose entry in row υ\upsilon and the column with channel index υ\upsilon' is 1{υ=υ}b~υ(St)\mathbf{1}_{\{\upsilon=\upsilon'\}}\,\sqrt{\tilde{b}^{\upsilon'}(S_t)}, with the indicator notation of the LQG data definition.

By the definitions of the matrix product and the transpose, for matrices MM and NN with mm^\circ columns each, the entry of MNMN^{\top} in row pp and column qq is c=1mMpcNqc\sum_{c=1}^{m^\circ}M^{pc}N^{qc}: a sum over the columns, the column cc contributing the product of its pp-th entry in MM and its qq-th entry in NN. Every nonzero column of ε(t)\varepsilon^\circ(t) has index among the first lll\cdot l and every nonzero column of ε~(t)\tilde{\varepsilon}^\circ(t) has index among the last l~\tilde{l}, so in ε(t)ε~(t)\varepsilon^\circ(t)\,\tilde{\varepsilon}^\circ(t)^{\top} every term of every entry has a factor 00: ε(t)ε~(t)=0\varepsilon^\circ(t)\,\tilde{\varepsilon}^\circ(t)^{\top}=0, the zero matrix with ll rows and l~\tilde{l} columns. In ε(t)ε(t)\varepsilon^\circ(t)\,\varepsilon^\circ(t)^{\top}, the column with index (σ,γ)(\sigma,\gamma), σγ\sigma\neq\gamma, contributes to the entry in row pp and column qq the term Stσβ(σ,γ,St,At)((eγeσ)(eγeσ))pqS^\sigma_t\,\beta(\sigma,\gamma,S_t,A_t)\,\big((e_\gamma-e_\sigma)(e_\gamma-e_\sigma)^{\top}\big)^{pq} --- the square of the square root being its argument --- and the remaining columns contribute 00; hence, summing over the ordered pairs and applying clause 1 (the jump representation) of the jump representation and positive semidefiniteness of the aggregate fluctuation covariance at the point (St,At)Δl×Rm(S_t,A_t)\in\Delta^l\times\mathbb{R}^m,

ε(t)ε(t)=(σ,γ):σγStσβ(σ,γ,St,At)(eγeσ)(eγeσ)=Θ(St,At)=Θt,\varepsilon^\circ(t)\,\varepsilon^\circ(t)^{\top}=\sum_{(\sigma,\gamma):\,\sigma\neq\gamma}S^\sigma_t\,\beta(\sigma,\gamma,S_t,A_t)\,(e_\gamma-e_\sigma)(e_\gamma-e_\sigma)^{\top}=\Theta(S_t,A_t)=\Theta^\star_t,

the last equality by clause 6 of the LQG data definition. In ε~(t)ε~(t)\tilde{\varepsilon}^\circ(t)\,\tilde{\varepsilon}^\circ(t)^{\top}, the entry in row υ\upsilon and column υ\upsilon'' is υ=1l~1{υ=υ}1{υ=υ}b~υ(St)=1{υ=υ}b~υ(St)\sum_{\upsilon'=1}^{\tilde{l}}\mathbf{1}_{\{\upsilon=\upsilon'\}}\mathbf{1}_{\{\upsilon''=\upsilon'\}}\,\tilde{b}^{\upsilon'}(S_t)=\mathbf{1}_{\{\upsilon=\upsilon''\}}\,\tilde{b}^{\upsilon}(S_t), which is the corresponding entry of Θ~t\tilde{\Theta}^\star_t by clause 7 of the LQG data definition: ε~(t)ε~(t)=Θ~t\tilde{\varepsilon}^\circ(t)\,\tilde{\varepsilon}^\circ(t)^{\top}=\tilde{\Theta}^\star_t.

For the continuity of the entries: every entry of tε(t)t\mapsto\varepsilon^\circ(t) and of tε~(t)t\mapsto\tilde{\varepsilon}^\circ(t) is either constantly 00 or of the form ±g\pm\sqrt{g} for the nonnegative function g(t)=Stσβ(σ,γ,St,At)g(t)=S^\sigma_t\,\beta(\sigma,\gamma,S_t,A_t), respectively g(t)=b~υ(St)g(t)=\tilde{b}^{\upsilon'}(S_t). The map tb~υ(St)t\mapsto\tilde{b}^{\upsilon'}(S_t) is continuous by conclusion 1. The components of t(St,At)t\mapsto(S_t,A_t) are continuous by clause 1 of the definition of a mean-field trajectory pair (part of the stationary triple setting); on Δl×Rm\Delta^l\times\mathbb{R}^m the rate β(σ,γ,,)\beta(\sigma,\gamma,\cdot,\cdot) agrees with the restriction of βˉ(σ,γ,,)\bar{\beta}(\sigma,\gamma,\cdot,\cdot) by clause 1 of the definition of the transition-rate extension, and βˉ(σ,γ,,)\bar{\beta}(\sigma,\gamma,\cdot,\cdot) is a C1C^1 map on U×RmU\times\mathbb{R}^m by clause 2 of that definition, hence continuous; so tβ(σ,γ,St,At)t\mapsto\beta(\sigma,\gamma,S_t,A_t) is continuous on [0,T][0,T] by continuity of compositions along the continuous map t(St,At)t\mapsto(S_t,A_t), applied pointwise on [0,T][0,T] exactly as in the definition of the fluctuation linear-quadratic cost, and tStσβ(σ,γ,St,At)t\mapsto S^\sigma_t\,\beta(\sigma,\gamma,S_t,A_t) is continuous by the sum and product rules for continuous real-valued functions. Finally, the nonnegative square root preserves continuity. For reals 0uv0\le u\le v one has uv\sqrt{u}\le\sqrt{v}, and for 0u<v0\le u<v one has u<v\sqrt{u}<\sqrt{v}: otherwise uv0\sqrt{u}\ge\sqrt{v}\ge0, respectively u>v0\sqrt{u}>\sqrt{v}\ge0, would give u=(u)2(v)2=vu=(\sqrt{u})^{2}\ge(\sqrt{v})^{2}=v, respectively u>vu>v. For reals x,y0x,y\ge0, xyx+y|\sqrt{x}-\sqrt{y}|\le\sqrt{x}+\sqrt{y}, both square roots being nonnegative, so

(xy)2xy(x+y)=(x)2(y)2=xy,\big(\sqrt{x}-\sqrt{y}\big)^{2}\le\big|\sqrt{x}-\sqrt{y}\big|\,\big(\sqrt{x}+\sqrt{y}\big)=\big|\big(\sqrt{x}\big)^{2}-\big(\sqrt{y}\big)^{2}\big|=|x-y|,

the middle equality by expanding the product of the difference and the sum of x\sqrt{x} and y\sqrt{y}; since xy|\sqrt{x}-\sqrt{y}| is the nonnegative square root of its own square, the monotonicity above yields xyxy|\sqrt{x}-\sqrt{y}|\le\sqrt{|x-y|}. Hence if g:[0,T]Rg:[0,T]\to\mathbb{R} is continuous with g0g\ge0 and t0[0,T]t_0\in[0,T], then for every real η>0\eta>0 there is a δ>0\delta>0 such that g(t)g(t0)<η2|g(t)-g(t_0)|<\eta^{2} for all t[0,T]t\in[0,T] with tt0<δ|t-t_0|<\delta, and then g(t)g(t0)g(t)g(t0)<η|\sqrt{g(t)}-\sqrt{g(t_0)}|\le\sqrt{|g(t)-g(t_0)|}<\eta by the strict monotonicity above: the map tg(t)t\mapsto\sqrt{g(t)} is continuous on [0,T][0,T]. Therefore all entries of ε\varepsilon^\circ and ε~\tilde{\varepsilon}^\circ are continuous on [0,T][0,T]; and since every Θ~t\tilde{\Theta}^\star_t is symmetric positive definite by conclusion 1, the displayed identities show that these assignments satisfy hypothesis (ii) of the statement and conditions (i) and (ii) of the model definition. This proves conclusion 3. \blacksquare

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