Reason: First published version. Under the additional hypothesis that the optimal mean-field trajectory is unique, the empirical state measure converges to it uniformly on the horizon in probability, with an explicit bound on the martingale contribution.
Assume in addition that the set Sσ∗ has exactly one element, and write S∗ for that element, so that Sσ∗={S∗}; it is a map on [0,T] with St∗∈Δl for every t∈[0,T], by claim 2 of the flow stability lemma.
For every natural number N let Ω∗N∈FN and MN be the event and the random variable furnished by the martingale bound for the empirical state measure, applied to the N-th solution: thus PN(Ω∗N)=1, the path t↦ΣtN(ω) is right-continuous at every t∈[0,T) for every ω∈Ω∗N, and
EN[(MN)2]≤N8l(l−1)BT.
Write 1Ω∗N for the function on ΩN equal to 1 on Ω∗N and to 0 elsewhere.
For a natural number n put
Qn={0}∪{2njT:j∈{1,…,2n}}⊆[0,T],
a finite nonempty set, where a natural number is read in R through its image in the real field. For natural numbers N and n let gnN be the map on ΩN given by
gnN(ω)=(max{ΣtN(ω)−St∗:t∈Qn})1Ω∗N(ω),
the maximum of a finite nonempty set of real numbers, and let
WN(ω)=sup{gnN(ω):n∈N}.
Then the following hold.
1. (The deviation measures the distance to the optimal trajectory.)S(σ,ζ)=S∗ for every ζ∈Mσ∗. Moreover, for every x0∈Δl and every ξ∈UA the supremum
sup{St(x0,ξ)−St∗:t∈[0,T]}
exists and is equal to D(x0,ξ).
2. (The uniform deviation is a random variable.) For all natural numbers N and n the map gnN is a random variable on (ΩN,FN,PN) with 0≤gnN(ω)≤2 for every ω∈ΩN. For every natural number N the supremum defining WN(ω) exists for every ω∈ΩN, and WN is a random variable with 0≤WN(ω)≤2 for every ω∈ΩN. Moreover, for every ω∈Ω∗N the supremum
sup{ΣtN(ω)−St∗:t∈[0,T]}
exists and is equal to WN(ω).
3. (Uniform convergence to the optimal trajectory in probability.) For every real ε>0 and every natural number N,
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