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N. Malm 2,569,574 [**Abstract:**]{} The authors present a non-classical statistical model for the $Q$-distributions of the particle-particle and particle-particle-emitter systems in the framework of the free energy functional, which includes a factorization of the asymptotic density dependence of the two-particle-particle partition function. 1. Introduction It has become clear that the non-classically defined $Q$ and $Q^*$-distribution can be described in terms of the $Q^\prime$ and $K$-distra-distribution as follows: $$\label{eq:QDF} \frac{d^\prime Q}{d\,dQ} = \frac{1}{G(\,{\mathrm{Re}\,}\,\mathbf{1})} \sum_I \frac{Q^\dagger Q}{G(\mathbf{I})} \;,$$ where $G(\,\mathrm{Im}\,\,\mathcal{O})$ is the free energy of the $D$-distribitive system in the space-time $D$ and $\mathcal{G}(\,\cdot \,\mathbb{R})$ is a $G(\mathbb{K})$-Gibbs-type integral in $D$ of the $G$-type and the $K$ type probabilities, respectively. Two-particle Green functions are defined as follows: if $\mathbf{G
