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Proof of Anchored Pre-Stopping Envelope and Restricted Moment Bounds for the State Fluctuation Process

lemmalem:fluctuation-anchored-envelope-2026a
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Reason: First publication: proof of the anchored pre-stopping envelope lemma.

Proof

Throughout, "the envelope lemma" is the pre-stopping envelope lemma, "the anchored lemma" is the anchored good-set clocks lemma, "the tracking lemma" is the pathwise tracking lemma, and "the covariation lemma" is the stopped covariation lemma for the martingale part. All notation is that of the statement; bt\mathfrak{b}_t and b=εY+Q\overline{\mathfrak{b}}=\varepsilon_Y+Q are the envelope and majorant of the envelope lemma.

Claim 1. Fix ωΩ0\omega\in\Omega_0 with Yt0(ω)<ε1Y_{t_0}(\omega)<\varepsilon_1 and t[t0,T]t\in[t_0,T], and put u=min(t,σ(ω))u=\min(t,\sigma^*(\omega)); then u[t0,T]u\in[t_0,T], since σ\sigma^* is [t0,T][t_0,T]-valued by claim 1 of the anchored lemma. By clause (vii)(a) of the existence and uniqueness theorem, Σu(ω)Δl\Sigma_u(\omega)\in\Delta^l and Σ0(ω)Δl\Sigma_0(\omega)\in\Delta^l. By the triangle inequality for the Euclidean norm,

Σu(ω)Su  Σu(ω)Su(Σ0(ω),α^(ω))+Su(Σ0(ω),α^(ω))Su(x0,α^(ω))+Yu(ω),|\Sigma_u(\omega)-S_u|\ \le\ \bigl|\Sigma_u(\omega)-S_u(\Sigma_0(\omega),\hat{\alpha}(\omega))\bigr|+\bigl|S_u(\Sigma_0(\omega),\hat{\alpha}(\omega))-S_u(x_0,\hat{\alpha}(\omega))\bigr|+Y_u(\omega),

since Su(x0,α^(ω))=Φu(ω)S_u(x_0,\hat{\alpha}(\omega))=\Phi_u(\omega) and Yu(ω)=Φu(ω)SuY_u(\omega)=|\Phi_u(\omega)-S^*_u| with S=SS^*=S. The first summand is at most Mu(ω)+ΛbeΛbuMu(ω)Mu(ω)+ΛbeΛbTMu(ω)|M_u(\omega)|+\Lambda_be^{\Lambda_bu}\mathcal{M}_u(\omega)\le|M_u(\omega)|+\Lambda_be^{\Lambda_bT}\mathcal{M}_u(\omega) by claim 2 of the tracking lemma (whose SωS^\omega is the flow S(Σ0(ω),α^(ω))S(\Sigma_0(\omega),\hat{\alpha}(\omega))) and the fact that the exponential function is nondecreasing. The second summand is at most eΛbTΣ0(ω)x0=eΛbTN1/2s0(ω)e^{\Lambda_bT}|\Sigma_0(\omega)-x_0|=e^{\Lambda_bT}N^{-1/2}|\mathfrak{s}_0(\omega)| by claim 4 of the flow stability lemma, applied with base pair (x0,α^(ω))(x_0,\hat{\alpha}(\omega)) and perturbed pair (Σ0(ω),α^(ω))(\Sigma_0(\omega),\hat{\alpha}(\omega)) — the perturbed control equals the base control, so every grγg^\gamma_r of claim 3 there vanishes and G=0G=0 is admissible — together with S0=x0S_0=x_0, which gives Σ0(ω)x0=N1/2s0(ω)|\Sigma_0(\omega)-x_0|=N^{-1/2}|\mathfrak{s}_0(\omega)|. The third summand is at most ε1\varepsilon_1: this is the stopped deviation bound of claim 2 of the anchored lemma, available since Yt0(ω)<ε1Y_{t_0}(\omega)<\varepsilon_1. Multiplying by N\sqrt{N} gives the first asserted inequality, su(ω)=NΣu(ω)Su|\mathfrak{s}_u(\omega)|=\sqrt{N}|\Sigma_u(\omega)-S_u|. For the second: by claim 1 of the envelope lemma, bs(ω)b(ω)\mathfrak{b}_s(\omega)\le\overline{\mathfrak{b}}(\omega) for every s[0,T]s\in[0,T], and by the definitions of b\mathfrak{b} and b\overline{\mathfrak{b}} this reads

Ms(ω)+ΛbeΛbTMs(ω)+eΛbTN1/2s0(ω)=bs(ω)εYb(ω)εY=Q(ω),|M_s(\omega)|+\Lambda_be^{\Lambda_bT}\mathcal{M}_s(\omega)+e^{\Lambda_bT}N^{-1/2}|\mathfrak{s}_0(\omega)|=\mathfrak{b}_s(\omega)-\varepsilon_Y\le\overline{\mathfrak{b}}(\omega)-\varepsilon_Y=Q(\omega),

so the first bound is at most N(ε1+Q(ω))\sqrt{N}(\varepsilon_1+Q(\omega)). In particular, for t<σ(ω)t<\sigma^*(\omega) one has u=tu=t, so 1{t<σ}(ω)st(ω)N(ε1+Q(ω))\mathbf{1}_{\{t<\sigma^*\}}(\omega)|\mathfrak{s}_t(\omega)|\le\sqrt{N}(\varepsilon_1+Q(\omega)); for tσ(ω)t\ge\sigma^*(\omega) the left side vanishes and the bound is trivial, QQ being nonnegative and ε1>Yt0(ω)0\varepsilon_1>Y_{t_0}(\omega)\ge0 on the event considered.

Claim 2. By claim 2 of the covariation lemma, each 1Ω0Σγ\mathbf{1}_{\Omega_0}\Sigma^\gamma is progressively measurable with respect to (Ftsys)t[0,T](\mathcal{F}^{\mathrm{sys}}_t)_{t\in[0,T]}, and σ\sigma^* is a stopping time of that filtration (claim 1 of the anchored lemma), so by claim 4 of the stopping-time toolkit the sampled function ω1Ω0(ω)Σmin(t,σ(ω))γ(ω)\omega\mapsto\mathbf{1}_{\Omega_0}(\omega)\Sigma^\gamma_{\min(t,\sigma^*(\omega))}(\omega) is a random variable; the function ωSmin(t,σ(ω))γ\omega\mapsto S^\gamma_{\min(t,\sigma^*(\omega))} is a random variable as the composition of the measurable map ωmin(t,σ(ω))\omega\mapsto\min(t,\sigma^*(\omega)) (for real qq, {min(t,σ)q}\{\min(t,\sigma^*)\le q\} is Ω\Omega or {σq}F\{\sigma^*\le q\}\in\mathcal{F}) with the continuous SγS^\gamma, by measurability of continuous functions of measurable maps; hence 1Ω0smin(t,σ)γ=N(1Ω0Σmin(t,σ)γ1Ω0Smin(t,σ)γ)\mathbf{1}_{\Omega_0}\mathfrak{s}^\gamma_{\min(t,\sigma^*)}=\sqrt{N}(\mathbf{1}_{\Omega_0}\Sigma^\gamma_{\min(t,\sigma^*)}-\mathbf{1}_{\Omega_0}S^\gamma_{\min(t,\sigma^*)}) and 1Ω0smin(t,σ)2\mathbf{1}_{\Omega_0}|\mathfrak{s}_{\min(t,\sigma^*)}|^2 are random variables by the same composition lemma. Likewise {s<σ}GsF\{s<\sigma^*\}\in\mathcal{G}_s\subseteq\mathcal{F} by claim 1 of the anchored lemma, and 1Ω01{s<σ}ss2\mathbf{1}_{\Omega_0}\mathbf{1}_{\{s<\sigma^*\}}|\mathfrak{s}_s|^2 is a random variable (1Ω0ssγ=N(1Ω0Σsγ1Ω0Ssγ)\mathbf{1}_{\Omega_0}\mathfrak{s}^\gamma_s=\sqrt{N}(\mathbf{1}_{\Omega_0}\Sigma^\gamma_s-\mathbf{1}_{\Omega_0}S^\gamma_s) being a random variable, since 1Ω0Σsγ\mathbf{1}_{\Omega_0}\Sigma^\gamma_s is Fssys\mathcal{F}^{\mathrm{sys}}_s-measurable by progressive measurability and claim 1 of the progressive measurability toolkit, and SsγS^\gamma_s is a constant). Finally Yt0Y_{t_0} is Gt0\mathcal{G}_{t_0}-measurable by claim 4 of the causality and adaptedness lemma, so {Yt0<ε1}Gt0\{Y_{t_0}<\varepsilon_1\}\in\mathcal{G}_{t_0}.

Claim 3. Let s,t[t0,T]s,t\in[t_0,T] and DFD\in\mathcal{F} with D{Yt0<ε1}D\subseteq\{Y_{t_0}<\varepsilon_1\}; DΩ0D\cap\Omega_0 consists of points ωΩ0\omega\in\Omega_0 with Yt0(ω)<ε1Y_{t_0}(\omega)<\varepsilon_1. By claim 1, at every point of DΩ0D\cap\Omega_0,

smin(t,σ)2N(ε1+Q)2and1{s<σ}ss2N(ε1+Q)2;|\mathfrak{s}_{\min(t,\sigma^*)}|^2\le N(\varepsilon_1+Q)^2\qquad\text{and}\qquad\mathbf{1}_{\{s<\sigma^*\}}|\mathfrak{s}_s|^2\le N(\varepsilon_1+Q)^2;

off DΩ0D\cap\Omega_0 the integrands 1D1Ω0smin(t,σ)2\mathbf{1}_{D}\mathbf{1}_{\Omega_0}|\mathfrak{s}_{\min(t,\sigma^*)}|^2 and 1D1Ω01{s<σ}ss2\mathbf{1}_{D}\mathbf{1}_{\Omega_0}\mathbf{1}_{\{s<\sigma^*\}}|\mathfrak{s}_s|^2 vanish, and 1DN(ε1+Q)2\mathbf{1}_{D}N(\varepsilon_1+Q)^2 is nonnegative. All integrands are random variables: claim 2; 1Ω0smin(t,σ)4=(1Ω0smin(t,σ)2)2\mathbf{1}_{\Omega_0}|\mathfrak{s}_{\min(t,\sigma^*)}|^4=(\mathbf{1}_{\Omega_0}|\mathfrak{s}_{\min(t,\sigma^*)}|^2)^2 is a random variable as the composition of the continuous map xx2x\mapsto x^2 with a random variable, by measurability of continuous functions of measurable maps; and QQ is a random variable by claim 2 of the envelope lemma, so (ε1+Q)2(\varepsilon_1+Q)^2 and (ε1+Q)4(\varepsilon_1+Q)^4 are random variables by the same composition lemma. All expectations below are finite: QQ is bounded (0QlKM+ΛbeΛbTlKMT+2eΛbT0\le Q\le\sqrt{l}K_M+\Lambda_be^{\Lambda_bT}\sqrt{l}K_MT+2e^{\Lambda_bT}, from MlKM\overline{M}\le\sqrt{l}K_M by claim 2 of the envelope lemma, 0IlKMT0\le I\le\sqrt{l}\,K_MT everywhere by part (b) of the restricted-moments lemma, and N1/2s02N^{-1/2}|\mathfrak{s}_0|\le2 as recorded in the preamble of the envelope lemma), and the left-hand integrands are bounded by 4N4N and, in the fourth-moment display below, by 16N216N^2: ΣuSuΣu+Su2|\Sigma_u-S_u|\le|\Sigma_u|+|S_u|\le2, the squared Euclidean norm of a point of Δl\Delta^l being at most its coordinate sum 11. Hence, by monotonicity of the expectation (linearity and monotonicity of the integral),

E[1D1Ω0smin(t,σ)2]NE[1D(ε1+Q)2],E[1D1Ω01{s<σ}ss2]NE[1D(ε1+Q)2].\mathbb{E}\bigl[\mathbf{1}_{D}\mathbf{1}_{\Omega_0}|\mathfrak{s}_{\min(t,\sigma^*)}|^2\bigr]\le N\,\mathbb{E}\bigl[\mathbf{1}_{D}(\varepsilon_1+Q)^2\bigr],\qquad\mathbb{E}\bigl[\mathbf{1}_{D}\mathbf{1}_{\Omega_0}\mathbf{1}_{\{s<\sigma^*\}}|\mathfrak{s}_s|^2\bigr]\le N\,\mathbb{E}\bigl[\mathbf{1}_{D}(\varepsilon_1+Q)^2\bigr].

Pointwise (ε1+Q)22ε12+2Q2(\varepsilon_1+Q)^2\le2\varepsilon_1^2+2Q^2, so, by the Cauchy-Schwarz inequality for the mean-square norm applied to 1D\mathbf{1}_{D} and Q2Q^2, together with E[1D2]=P(D)\mathbb{E}[\mathbf{1}_{D}^2]=P(D) and E[Q4]cQκ0N2\mathbb{E}[Q^4]\le c_Q\kappa_0N^{-2} (claim 2 of the envelope lemma),

E[1D(ε1+Q)2]2ε12P(D)+2E[1DQ2]2ε12P(D)+2cQ1/2κ01/2N1P(D)1/2;\mathbb{E}\bigl[\mathbf{1}_{D}(\varepsilon_1+Q)^2\bigr]\le2\varepsilon_1^2P(D)+2\,\mathbb{E}\bigl[\mathbf{1}_{D}Q^2\bigr]\le2\varepsilon_1^2P(D)+2\,c_Q^{1/2}\kappa_0^{1/2}N^{-1}P(D)^{1/2};

multiplying by NN gives the second-moment bounds. For the fourth moments: applying (a+b)22(a2+b2)(a+b)^2\le2(a^2+b^2) twice gives (ε1+Q)48ε14+8Q4(\varepsilon_1+Q)^4\le8\varepsilon_1^4+8Q^4 pointwise, and squaring the envelope of claim 1 twice gives smin(t,σ)4N2(ε1+Q)4|\mathfrak{s}_{\min(t,\sigma^*)}|^4\le N^2(\varepsilon_1+Q)^4 on DΩ0D\cap\Omega_0, so

E[1D1Ω0smin(t,σ)4]N2E[1D(ε1+Q)4]N2(8ε14P(D)+8E[Q4])8N2ε14P(D)+8cQκ0.\mathbb{E}\bigl[\mathbf{1}_{D}\mathbf{1}_{\Omega_0}|\mathfrak{s}_{\min(t,\sigma^*)}|^4\bigr]\le N^2\,\mathbb{E}\bigl[\mathbf{1}_{D}(\varepsilon_1+Q)^4\bigr]\le N^2\bigl(8\varepsilon_1^4P(D)+8\,\mathbb{E}[Q^4]\bigr)\le8N^2\varepsilon_1^4P(D)+8\,c_Q\,\kappa_0 . \qquad\blacksquare
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