Claim 1. Fix ω∈Ω0. By condition 1 of the definition of a solution, each state path t↦σti(ω) is constant on each of finitely many intervals partitioning [0,T], so each occupation indicator t↦ηti,γ(ω), and hence t↦Σtγ(ω)=N1∑iηti,γ(ω), is a finite linear combination of indicator functions of intervals; intervals belong to the trace Borel σ-algebra, so these paths are measurable by measurability of sums and scalar multiples of measurable functions (indicators of measurable sets being measurable), and they take values in [0,1]. The path s↦bγ(Σs(ω),αs(ω)) is measurable and bounded in absolute value by 2(l−1)B by part (a) of the martingale decomposition theorem, so by part (i) of the integration-by-parts lemma (applied with that path as its first integrand, the second integrand and both initial values taken to be 0; every later use of part (i) in this proof is of the same form) the map t↦∫[0,t]bγ(Σs(ω),αs(ω))ds is continuous on [0,T], hence measurable by claim 3 of the toolkit, and it is bounded in absolute value by 2(l−1)BT by monotonicity. Since 1Ω0(ω)=1, part (b) of the martingale decomposition theorem gives Mtγ(ω)=Σtγ(ω)−Σ0γ(ω)−∫[0,t]bγ(Σs(ω),αs(ω))ds, a measurable function of t with ∣Mtγ(ω)∣≤1+2(l−1)BT≤KM. The path t↦∣Mt(ω)∣ is a continuous function of the measurable component paths, hence measurable by measurability of continuous functions of measurable maps, and ∣Mt(ω)∣≤lKM. Thus Mt(ω) exists for every t; and for r≤t we have Mr(ω)≤Mt(ω), because by claim 2 of the toolkit both integrals are integrals over R of zero extensions, that of the restriction to [0,r] being dominated pointwise by that of the restriction to [0,t].
Claim 2. Fix ω∈Ω0 and write ξ=α^(ω)∈UA and u=α^(⋅,ω), an admissible representative of ξ by claim 3 of the realized-control lemma, with u(s)=αs(ω) for every s∈[0,T] by claim 2 of the same lemma since ω∈Ω0. By claim 2 of the flow stability lemma, Sω=S(Σ0(ω),ξ) is the map furnished by claim 1 of the existence and uniqueness theorem for the initial value Σ0(ω) and the control u: it is continuous, takes values in Δl, and satisfies Stω,γ=Σ0γ(ω)+∫[0,t]b^γ(Ssω,u(s))ds for all t and γ, where b^(x,a)=b(x,a) for x∈Δl by claim 6 of the affine-rate lemma. Subtracting this from the decomposition of Claim 1 and writing yt=Σt(ω)−Stω, we get, for every t and γ,
The integrand vector s↦b(Σs,αs)−b(Ssω,αs) has bounded measurable components (the first summand is measurable as in Claim 1; the second by the composition lemma applied to bγ, which is sequentially continuous on Δl×A by the two Lipschitz bounds of claim 4 of the affine-rate lemma, and to s↦(Ssω,u(s)), whose components are measurable because Sω is continuous and u is a square-integrable, hence measurable, path by claim 3 of the realized-control lemma), so by the norm bound for vector-valued integrals and the state-Lipschitz bound of claim 4 of the affine-rate lemma,
∣yt∣≤∣Mt(ω)∣+∫[0,t]Λb∣ys∣ds(t∈[0,T]).(∗)
Here s↦∣ys∣ is measurable (a continuous function of measurable components) and bounded by 2. Put v(t)=∫[0,t]∣ys∣ds; by part (i) of the integration-by-parts lemma v is continuous on [0,T]. Integrating (∗) over [0,t] and using monotonicity gives v(t)≤Mt(ω)+Λb∫[0,t]v(s)ds for every t. Now fix t∈(0,T]. For s∈[0,t], Claim 1 gives Ms(ω)≤Mt(ω), hence
v(s)≤Mt(ω)+Λb∫[0,s]v(r)dr(0≤s≤t).
The restriction of v to [0,t] is continuous by claim 1 of restriction stability, and for a continuous function the Riemann and Lebesgue integrals over [0,s] agree by claim 3 of the toolkit. Hence Gronwall's lemma on the interval [0,t] — with, in the notation of that lemma, its function taken to be v∣[0,t] and its two constants taken to be Mt(ω) and Λb≥0; the letters u and b retain their meanings above — yields v(s)≤Mt(ω)exp(Λbs) for s∈[0,t], in particular v(t)≤Mt(ω)exp(Λbt). Inserting this into (∗) proves Claim 2 for t∈(0,T]; for t=0 both sides vanish, since y0=0 and M0=0.
with y as in Claim 2. The function t↦Mt(ω) is continuous on [0,T] (part (i) of the integration-by-parts lemma), so t↦exp(Λbt)Mt(ω) is continuous, hence integrable, and bounded by exp(ΛbT)MT(ω) by Claim 1. Integrating the bound of Claim 2 therefore gives ∫[0,T]∣yt∣dt≤MT(ω)+ΛbTexp(ΛbT)MT(ω)=ΓMT(ω), while Claim 2 at t=T gives ∣yT∣≤∣MT(ω)∣+Λbexp(ΛbT)MT(ω). Substituting proves Claim 3.
The estimate. Fix ω∈Ω, and let ξ=α^(ω) and u=α^(⋅,ω), an admissible representative of ξ by claim 3 of the realized-control lemma (this holds at every ω∈Ω). Apply claim 4 of the flow stability lemma with x0=Σ0(ω), x0′=z0, and ξ′=ξ: the functionals of claim 3 there satisfy grγ(ξ′)=⟨ξ−ξ,wγ,r⟩L2=0, so the slack constant of claim 4 (written G in that lemma, a letter that here denotes the terminal cost) may be taken to be 0, and ∣St(z0,ξ)−St(Σ0(ω),ξ)∣≤exp(ΛbT)∣z0−Σ0(ω)∣ for every t∈[0,T]. By the definition of F with the representative u for both initial states,
and (LipC) with monotonicity bounds the absolute value of the right-hand side by KLTexp(ΛbT)∣Σ0(ω)−z0∣+KGexp(ΛbT)∣Σ0(ω)−z0∣, which is the asserted estimate. ■