Abstract

The goal of this paper is to provide mathematically rigorous tools for modelling the evolution of a community of interacting individuals. We model the population by a measure space where the measure determines the abundance of individual preferences. The preferences of an individual are described by a measurable choice of a rough path. We focus on the case of weakly interacting systems, where we are able to exhibit the existence and uniqueness of consistent solutions. In general, solutions are continuum of interacting threads analogous to the huge number of individual atomic trajectories that together make up the motion of a fluid. The evolution of the population need not be governed by any over-arching PDE. Although one can match the standard nonlinear parabolic PDEs of McKean-Vlasov type with specific examples of communities in this case. The bulk behaviour of the evolving population provides a solution to the PDE. An important technical result is continuity of the behaviour of the system with respect to changes in the measure assigning weight to individuals. Replacing the deterministic measure with the empirical distribution of an i.i.d. sample from it leads to many standard models, and applying the continuity result allows easy proofs for propagation of chaos. The rigorous underpinning presented here leads to uncomplicated models which have wide applicability in both the physical and social sciences. We make no presumption that the macroscopic dynamics are modelled by a PDE. This work builds on the fine probability literature considering the limit behaviour for systems where a large no of particles are interacting with independent preferences; there is also work on continuum models with preferences described by a semi-martingale measure. We mention some of the key papers.

Highlights

  • In the Vlasov [31] approach to continuum mechanics, the macroscopic behaviour of a cloud of interacting particles is approximated by a single differential equation

  • We have a community of individuals evolving according to their individual preferences in a way that is consistent with the dynamics of the population as a whole

  • We will later want to consider the propagation of chaos phenomenon for rough differential equations, and this requires us to present the treatment of the previous subsection for a population of particles of arbitrary finite size N

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Summary

Introduction

In the Vlasov [31] approach to continuum mechanics, the macroscopic behaviour of a cloud of interacting particles is approximated by a single (non-linear) differential equation. It makes complete sense to ask whether there is a choice t → μt so that the resultant measure path t → μt does coincide with it In this case, we have a community of individuals evolving according to their individual preferences in a way that is consistent with the dynamics of the population as a whole. The methodology here is distinct from that used later to prove the (more general) result for non-discrete measures This simple case allows us to see very clearly how the weak interaction assumption, combined with the Lyons-Victoir (LV) Extension Theorem of [26] gives rise to the uniqueness of fixed points. We note that this paper has already lead to follow-up work (see, for example, [1]); we discuss other possible applications of our results

Preliminaries on rough path theory
Weakly interacting communities
A two-particle system
N-particle systems
A fixed point and continuity theorem
Measure-valued paths
A fixed-point theorem
Continuity in ν
Applications
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