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Proof of The Good-Set Stopping Time of the Realized Control: Flow Deviation and Control Energy

lemmalem:good-set-stopping-time-2026a
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Reason: Proof of the good-set stopping time lemma: hitting times of the adapted continuous deviation and energy processes, bounds before and at the stopping time by continuity, and the early-stopping inclusions.

Proof

Claim 1. By claim 4 of Causality of the Mean-Field Flow and Observation-Adaptedness of the Realized Mean-Field Flow, the family Y=(Yt)t[0,T]Y=(Y_t)_{t\in[0,T]} is adapted to (Gt)t[0,T](\mathcal{G}_t)_{t\in[0,T]} with every path continuous on [0,T][0,T]; by claim 5 of Progressive Measurability of the Realized Control with Respect to the Observation Filtration, so is E=(Et)t[0,T]\mathcal{E}=(\mathcal{E}_t)_{t\in[0,T]}. Hence τY\tau_Y and τE\tau_{\mathcal{E}}, which are the hitting times of claim 5 of Stopping Times on a Compact Time Interval: Elementary Operations, the Prior Sigma-Algebra, Dyadic Approximation, Sampling, and Hitting Times for YY with level c=εYc=\varepsilon_Y and for E\mathcal{E} with level c=cEc=c_{\mathcal{E}}, are stopping times of (Gt)t[0,T](\mathcal{G}_t)_{t\in[0,T]}, and so is their pointwise minimum τ\tau by claim 1 of the same toolkit. Since GtFtsys\mathcal{G}_t\subseteq\mathcal{F}^{\mathrm{sys}}_t for every tt (claim 1 of Progressive Measurability of the Realized Control with Respect to the Observation Filtration), the defining condition {θt}Gt\{\theta\le t\}\in\mathcal{G}_t of a stopping time implies {θt}Ftsys\{\theta\le t\}\in\mathcal{F}^{\mathrm{sys}}_t, so all three are stopping times of (Ftsys)t[0,T](\mathcal{F}^{\mathrm{sys}}_t)_{t\in[0,T]} as well. The membership {τt}Gt\{\tau\le t\}\in\mathcal{G}_t is the definition, {t<τ}={τ>t}Gt\{t<\tau\}=\{\tau>t\}\in\mathcal{G}_t is claim 1 of the toolkit, and {τ<T}GT\{\tau<T\}\in\mathcal{G}_T is the same claim with t=Tt=T.

Claim 2. Let ωΩ\omega\in\Omega and t<τ(ω)t<\tau(\omega). Then t<τY(ω)t<\tau_Y(\omega) and t<τE(ω)t<\tau_{\mathcal{E}}(\omega), so claim 5 of Stopping Times on a Compact Time Interval: Elementary Operations, the Prior Sigma-Algebra, Dyadic Approximation, Sampling, and Hitting Times gives Yt(ω)<εYY_t(\omega)<\varepsilon_Y and Et(ω)<cE\mathcal{E}_t(\omega)<c_{\mathcal{E}}.

For the bounds at the stopping time we first show: if E0(ω)<cE\mathcal{E}_0(\omega)<c_{\mathcal{E}} then EτE(ω)(ω)cE\mathcal{E}_{\tau_{\mathcal{E}}(\omega)}(\omega)\le c_{\mathcal{E}}. If HE(ω)=H_{\mathcal{E}}(\omega)=\emptyset then τE(ω)=T\tau_{\mathcal{E}}(\omega)=T and ET(ω)<cE\mathcal{E}_T(\omega)<c_{\mathcal{E}}. Otherwise θ=τE(ω)\theta=\tau_{\mathcal{E}}(\omega) is the greatest lower bound of HE(ω)H_{\mathcal{E}}(\omega), so no u<θu<\theta lies in HE(ω)H_{\mathcal{E}}(\omega), that is, Eu(ω)<cE\mathcal{E}_u(\omega)<c_{\mathcal{E}} for every u[0,θ)u\in[0,\theta). Suppose Eθ(ω)>cE\mathcal{E}_\theta(\omega)>c_{\mathcal{E}}. Then θ>0\theta>0, since E0(ω)<cE\mathcal{E}_0(\omega)<c_{\mathcal{E}}; by continuity of the path at θ\theta relative to [0,T][0,T], applied with ε=Eθ(ω)cE>0\varepsilon=\mathcal{E}_\theta(\omega)-c_{\mathcal{E}}>0, there is δ>0\delta>0 with Eu(ω)>cE\mathcal{E}_u(\omega)>c_{\mathcal{E}} for every u[0,T]u\in[0,T] with uθ<δ|u-\theta|<\delta, and any u(max(0,θδ),θ)u\in(\max(0,\theta-\delta),\theta) gives a contradiction. Hence Eθ(ω)cE\mathcal{E}_\theta(\omega)\le c_{\mathcal{E}}. The same argument with YY, εY\varepsilon_Y, HY(ω)H_Y(\omega) and τY(ω)\tau_Y(\omega) in place of E\mathcal{E}, cEc_{\mathcal{E}}, HE(ω)H_{\mathcal{E}}(\omega) and τE(ω)\tau_{\mathcal{E}}(\omega) shows: if Y0(ω)<εYY_0(\omega)<\varepsilon_Y then YτY(ω)(ω)εYY_{\tau_Y(\omega)}(\omega)\le\varepsilon_Y.

Now E0(ω)=0<cE\mathcal{E}_0(\omega)=0<c_{\mathcal{E}} by the definition of E\mathcal{E} (the integral over [0,0][0,0] being 00). Let t[0,T]t\in[0,T] and s=min(t,τ(ω))s=\min(t,\tau(\omega)). If s<τE(ω)s<\tau_{\mathcal{E}}(\omega) then Es(ω)<cE\mathcal{E}_s(\omega)<c_{\mathcal{E}} by claim 5 of the toolkit; otherwise s=τ(ω)=τE(ω)s=\tau(\omega)=\tau_{\mathcal{E}}(\omega), since sτ(ω)τE(ω)s\le\tau(\omega)\le\tau_{\mathcal{E}}(\omega), and Es(ω)cE\mathcal{E}_s(\omega)\le c_{\mathcal{E}} by the display just proved. If moreover x0S0<εY|x_0-S^*_0|<\varepsilon_Y, then Y0(ω)=Φ0(ω)S0=x0S0<εYY_0(\omega)=|\Phi_0(\omega)-S^*_0|=|x_0-S^*_0|<\varepsilon_Y by claim 3 of Causality of the Mean-Field Flow and Observation-Adaptedness of the Realized Mean-Field Flow, and the same dichotomy with τY\tau_Y in place of τE\tau_{\mathcal{E}} gives Ys(ω)εYY_s(\omega)\le\varepsilon_Y.

Claim 3. Since τ=min(τY,τE)\tau=\min(\tau_Y,\tau_{\mathcal{E}}) pointwise, τ(ω)<T\tau(\omega)<T holds exactly when τY(ω)<T\tau_Y(\omega)<T or τE(ω)<T\tau_{\mathcal{E}}(\omega)<T, which is the stated identity. If τY(ω)<T\tau_Y(\omega)<T then HY(ω)H_Y(\omega)\neq\emptyset, so some t[0,T]t\in[0,T] has Yt(ω)εYY_t(\omega)\ge\varepsilon_Y, and Y(ω)Yt(ω)εY\overline{Y}(\omega)\ge Y_t(\omega)\ge\varepsilon_Y, the supremum existing by claim 4 of Causality of the Mean-Field Flow and Observation-Adaptedness of the Realized Mean-Field Flow. If τE(ω)<T\tau_{\mathcal{E}}(\omega)<T then HE(ω)H_{\mathcal{E}}(\omega)\neq\emptyset, so some tt has Et(ω)cE\mathcal{E}_t(\omega)\ge c_{\mathcal{E}}, and ET(ω)Et(ω)cE\mathcal{E}_T(\omega)\ge\mathcal{E}_t(\omega)\ge c_{\mathcal{E}} because the paths of E\mathcal{E} are nondecreasing by claim 5 of Progressive Measurability of the Realized Control with Respect to the Observation Filtration. If τY(ω)=T\tau_Y(\omega)=T, then either HY(ω)=H_Y(\omega)=\emptyset, in which case Yt(ω)<εYY_t(\omega)<\varepsilon_Y for every tt, or HY(ω)H_Y(\omega)\neq\emptyset with greatest lower bound TT, in which case HY(ω)={T}H_Y(\omega)=\{T\} (every element of HY(ω)[0,T]H_Y(\omega)\subseteq[0,T] being at least its greatest lower bound TT) and Yt(ω)<εYY_t(\omega)<\varepsilon_Y for t<Tt<T while YT(ω)εYY_T(\omega)\ge\varepsilon_Y; in the second case, continuity of the path at TT relative to [0,T][0,T] forces YT(ω)εYY_T(\omega)\le\varepsilon_Y, for if YT(ω)>εYY_T(\omega)>\varepsilon_Y there would be δ>0\delta>0 with Yt(ω)>εYY_t(\omega)>\varepsilon_Y for all t(Tδ,T]t\in(T-\delta,T], contradicting Yt(ω)<εYY_t(\omega)<\varepsilon_Y for t<Tt<T. In both cases Yt(ω)εYY_t(\omega)\le\varepsilon_Y for every tt, so Y(ω)εY\overline{Y}(\omega)\le\varepsilon_Y.

The three sets on the right lie in GT\mathcal{G}_T because Y\overline{Y} is GT\mathcal{G}_T-measurable (claim 4 of Causality of the Mean-Field Flow and Observation-Adaptedness of the Realized Mean-Field Flow) and ET\mathcal{E}_T is GT\mathcal{G}_T-measurable (claim 5 of Progressive Measurability of the Realized Control with Respect to the Observation Filtration), indeed {YεY}\{\overline{Y}\le\varepsilon_Y\} is the complement of {Y>εY}GT\{\overline{Y}>\varepsilon_Y\}\in\mathcal{G}_T, and {YεY}=n1{Y>εY1/n}\{\overline{Y}\ge\varepsilon_Y\}=\bigcap_{n\ge1}\{\overline{Y}>\varepsilon_Y-1/n\} with every member in GT\mathcal{G}_T, both by the criterion of claim 3 of Rational Intervals and Rays Generate the Borel Sigma-Algebra of the Real Line; likewise for {ETcE}\{\mathcal{E}_T\ge c_{\mathcal{E}}\}. Finally {τ<T}{YεY}{ETcE}\{\tau<T\}\subseteq\{\overline{Y}\ge\varepsilon_Y\}\cup\{\mathcal{E}_T\ge c_{\mathcal{E}}\} by the inclusions just proved, and the probability of a union of two events is at most the sum of their probabilities, by monotonicity (claim 2) and countable subadditivity (claim 4, the sequence padded with the empty set) of Basic Properties of a Measure; this is the final display. \blacksquare

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