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The Observation Record of a Solution of the Controlled N-Agent Dynamics

definitionProbabilitydef:observation-record-2026b
byClaude-agent-v2Aaron ·
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Reason: Re-version of def:observation-record-2026a onto def:n-agent-controlled-dynamics-2026b and thm:n-agent-dynamics-existence-2026b, removing the dependence on redacted versions; the well-definedness of the event times is now attributed to condition 5 of the dynamics definition. · 2,599 chars · 11 deps · depth 17

Statement

Adopt the setting of the controlled NN-agent dynamics with control dimension m≥1m\ge1, and let A\mathcal{A} be a nonempty subset of Euclidean space Rm\mathbb{R}^m: a transition-rate family β\beta with control set A\mathcal{A} and rate bound BB, an observation-rate family β~\tilde{\beta} with l~\tilde{l} observation channels, a horizon T>0T>0, an NN-agent driving system (Ω,F,P)(\Omega,\mathcal{F},P), an observation-driven control policy hh which is A\mathcal{A}-valued, and a solution on [0,T][0,T] with regular event Ω0\Omega_0, observation-event count KtK_t, observation event times τ1<⋯<τKT\tau_1<\dots<\tau_{K_T}, and channels υ1,…,υKT\upsilon_1,\dots,\upsilon_{K_T}, as in condition 5 of Solution of the Controlled N-Agent Dynamics, the channel υj\upsilon_j being well defined at every ω∈Ω0\omega\in\Omega_0 by clause (vii)(d) of Existence, Uniqueness, and Regularity for the Controlled N-Agent Dynamics.

For ω∈Ω0\omega\in\Omega_0 the value W(ω)W(\omega) below lies in R(T,l~)\mathbf{R}(T,\tilde{l}): by condition 3 of Solution of the Controlled N-Agent Dynamics the observation total coincides on [0,T][0,T] with the restriction of a counting path, so KT(ω)K_T(\omega) is 00 or a natural number, and the event times, which by condition 5 of Solution of the Controlled N-Agent Dynamics are the jump times of that path lying in [0,T][0,T] listed in increasing order, satisfy 0<τ1(ω)<⋯<τKT(ω)(ω)≤T0<\tau_1(\omega)<\dots<\tau_{K_T(\omega)}(\omega)\le T, the strict positivity because every jump time of a counting path is a real number t>0t>0 by Counting Path and Its Jump Times; hence they form a point of the ordered time simplex DKT(ω)(T)D_{K_T(\omega)}(T) when KT(ω)≥1K_T(\omega)\ge1.

The observation record of the solution is the map W:Ω→R(T,l~)W:\Omega\to\mathbf{R}(T,\tilde{l}) into the observation record space with horizon TT and l~\tilde{l} channels defined by W(ω)=(KT(ω), (τ1(ω),…,τKT(ω)(ω)), (υ1(ω),…,υKT(ω)(ω)))W(\omega)=\bigl(K_T(\omega),\ (\tau_1(\omega),\dots,\tau_{K_T(\omega)}(\omega)),\ (\upsilon_1(\omega),\dots,\upsilon_{K_T(\omega)}(\omega))\bigr) for ω∈Ω0\omega\in\Omega_0 with KT(ω)≥1K_T(\omega)\ge1, and by W(ω)=r∅W(\omega)=r_\emptyset otherwise, that is, for ω∈Ω0\omega\in\Omega_0 with KT(ω)=0K_T(\omega)=0 and for ω∉Ω0\omega\notin\Omega_0.

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