TheoremBase

Fluctuation Processes of the Controlled N-Agent Dynamics

Statement

Adopt the setting of the controlled NN-agent dynamics with NN agents, ll states, l~\tilde{l} observation channels, and control dimension mm, and let A\mathcal{A} be a nonempty subset of Euclidean space Rm\mathbb{R}^m: a transition-rate family Ξ²\beta on ll states with control set A\mathcal{A} and rate bound BB, an observation-rate family Ξ²~\tilde{\beta} on ll states with l~\tilde{l} channels and rate bound B~\tilde{B}, a horizon T>0T>0, an NN-agent driving system (Ξ©,F,P)(\Omega,\mathcal{F},P), an observation-driven control policy hh which is A\mathcal{A}-valued, and a solution ((Οƒi)i=1N,(Ξ₯Ο…)Ο…=1l~,Ξ±)((\sigma^i)_{i=1}^N,(\Upsilon^\upsilon)_{\upsilon=1}^{\tilde{l}},\alpha) on [0,T][0,T] for these data, with empirical state measure Ξ£t\Sigma_t and control process Ξ±t\alpha_t. Let (S,A)(S,A) be a mean-field trajectory pair for Ξ²\beta with horizon TT (so that At∈AA_t\in\mathcal{A} for every t∈[0,T]t\in[0,T]), and write N\sqrt{N} for the nonnegative square root of NN.

The fluctuation processes of the solution about (S,A)(S,A) are the pair of families (st)t∈[0,T](\mathfrak{s}_t)_{t\in[0,T]} and (at)t∈[0,T](\mathfrak{a}_t)_{t\in[0,T]} defined componentwise by

stΞ³=N (Ξ£tΞ³βˆ’StΞ³)(γ∈{1,…,l}),atj=N (Ξ±tjβˆ’Atj)(j∈{1,…,m}),\mathfrak{s}^\gamma_t=\sqrt{N}\,\big(\Sigma^\gamma_t-S^\gamma_t\big)\quad(\gamma\in\{1,\dots,l\}),\qquad\qquad \mathfrak{a}^j_t=\sqrt{N}\,\big(\alpha^j_t-A^j_t\big)\quad(j\in\{1,\dots,m\}),

written st=N(Ξ£tβˆ’St)\mathfrak{s}_t=\sqrt{N}(\Sigma_t-S_t) and at=N(Ξ±tβˆ’At)\mathfrak{a}_t=\sqrt{N}(\alpha_t-A_t) as Rl\mathbb{R}^l-valued and Rm\mathbb{R}^m-valued maps on the underlying probability space; (st)t∈[0,T](\mathfrak{s}_t)_{t\in[0,T]} is called the state fluctuation process and (at)t∈[0,T](\mathfrak{a}_t)_{t\in[0,T]} the control fluctuation process.

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