TheoremBase

Generalized Mean-Field Trajectory Pair

Statement

Let (β0,β1)(\beta_0,\beta_1) be an affine-controlled transition-rate family on ll states with control set A⊆Rm\mathcal{A}\subseteq\mathbb{R}^m, let bb be the aggregate state drift of its transition-rate family, with rate bound BB, let Δl\Delta^l be the probability simplex, and let T>0T>0 be a real number, called the horizon.

A generalized mean-field trajectory pair for (β0,β1)(\beta_0,\beta_1) with horizon TT is a pair (S,A)(S,A) of maps S:[0,T]→ΔlS:[0,T]\to\Delta^l and A:[0,T]→AA:[0,T]\to\mathcal{A}, with values written St=(St1,…,Stl)S_t=(S^1_t,\dots,S^l_t) and At=(At1,…,Atm)A_t=(A^1_t,\dots,A^m_t), such that:

1. (Regularity.) Every component t↦Stγt\mapsto S^\gamma_t is continuous on [0,T][0,T], the interval being regarded as a subset of the real line with the absolute value metric and R\mathbb{R} carrying the same metric, and every component t↦Atjt\mapsto A^j_t is measurable with respect to the trace Borel σ\sigma-algebra on [0,T][0,T] and the Borel σ\sigma-algebra on the real line.

2. (Dynamics.) For every γ∈{1,…,l}\gamma\in\{1,\dots,l\} and every t∈[0,T]t\in[0,T],

Stγ=S0γ+∫[0,t]bγ(Ss,As) ds,S^\gamma_t=S^\gamma_0+\int_{[0,t]}b^\gamma(S_s,A_s)\,ds ,

the integral being the Lebesgue integral over the compact interval [0,t][0,t], and 00 for t=0t=0.

Under condition 1 the integrand is measurable and bounded by 2l(l−1)B2\sqrt{l}(l-1)B, so the integral exists; this follows from measurability of continuous functions, measurability of sequentially continuous functions of measurable Euclidean maps, and the bounds of the lemma on affine-controlled data.

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