TheoremBase

The Optimal Value, the Optimal Controls and the Optimal Trajectories of the Mean-Field Problem

Statement

Adopt the setting, hypotheses and notation of the boundedness, lower semicontinuity and attainment theorem for the mean-field cost: the affine-controlled transition-rate family (β0,β1)(\beta_{0},\beta_{1}) on ll states with control set A⊆Rm\mathcal{A}\subseteq\mathbb{R}^{m}, the horizon T>0T>0, the population cost data (L,G)(L,G) with LL convex in the control on A\mathcal{A}, the probability simplex Δl\Delta^{l}, the set UA\mathcal{U}_{\mathcal{A}} of A\mathcal{A}-valued controls with the metric ρ\rho, the mean-field flow S(z0,ξ)S(z_{0},\xi), for z0∈Δlz_{0}\in\Delta^{l} and ξ∈UA\xi\in\mathcal{U}_{\mathcal{A}}, of claim 2 of the flow stability lemma, and the mean-field cost FF.

Let x0∈Δlx_{0}\in\Delta^{l}, called the initial state of the problem. Put

Vx0={F(x0,ξ)  :  ξ∈UA}⊆R.V_{x_{0}}=\bigl\{F(x_{0},\xi)\;:\;\xi\in\mathcal{U}_{\mathcal{A}}\bigr\}\subseteq\mathbb{R}.

By claim 5 of that theorem there is at least one element of UA\mathcal{U}_{\mathcal{A}}, so Vx0V_{x_{0}} is nonempty; and by claim 1 of that theorem ∣F(x0,ξ)∣≤CF|F(x_{0},\xi)|\le C_{F} for every ξ∈UA\xi\in\mathcal{U}_{\mathcal{A}}, so by claim 6 of Properties of the Absolute Value in an Ordered Field we have −CF≤F(x0,ξ)-C_{F}\le F(x_{0},\xi) for every such ξ\xi, that is, the number −CF-C_{F} is a lower bound of Vx0V_{x_{0}}. Hence the infimum of Vx0V_{x_{0}} exists by Existence of the Infimum of a Nonempty Subset of R\mathbb{R} Bounded Below and is unique by Uniqueness of the Supremum and of the Infimum.

The optimal mean-field value from x0x_{0} is the real number

Jx0∗=inf⁡Vx0.J^{*}_{x_{0}}=\inf V_{x_{0}}.

The set of optimal mean-field controls from x0x_{0} is

Mx0∗={ξ∈UA  :  F(x0,ξ)=Jx0∗}.\mathcal{M}^{*}_{x_{0}}=\bigl\{\xi\in\mathcal{U}_{\mathcal{A}}\;:\;F(x_{0},\xi)=J^{*}_{x_{0}}\bigr\}.

The set of optimal mean-field trajectories from x0x_{0} is

Sx0∗={S(x0,ξ)  :  ξ∈Mx0∗}.\mathcal{S}^{*}_{x_{0}}=\bigl\{S(x_{0},\xi)\;:\;\xi\in\mathcal{M}^{*}_{x_{0}}\bigr\}.

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