Nearly periodic slow motion in deterministic fully coupled averaging

Let w(r)w_{-}(r) and w+(r)w_{+}(r) be strictly increasing and decreasing functions, respectively, satisfying

R12(w(r))=R21(w+(r))=r.R_{12}(w_{-}(r))=R_{21}(w_{+}(r))=r.

Suppose that w(λ)=w+(λ)=ww_{-}(\frac{}{\lambda})=w_{+}(\lambda)=w^* for some λ>0\lambda>0, with w(r)<w<w+(r)w_{-}(r)<w^*<w_{+}(r) for r<λr<\lambda. Assume that δ0\delta\to0 and ε0\varepsilon\to0 so that

limε,δ0εln(δε)=ρ>λ.\lim_{\varepsilon,\delta\to0}\varepsilon\ln(\delta\varepsilon)=-\rho>-\lambda.

For the slowest motion W~w,x,yε,δ\tilde W^{\varepsilon,\delta}_{w,x,y}, and for every w,xw,x, there exists t0>0t_0>0 such that W~w,x,yε,δ(t+t0)\tilde W^{\varepsilon,\delta}_{w,x,y}(t+t_0), t0t\geq0, converges weakly as a random process on (W,mW)({\mathcal W},m_{\mathcal W}) to a periodic function ψ(t)\psi(t) satisfying ψ(t+T)=ψ(t)\psi(t+T)=\psi(t), where

T=T(ρ)=w(ρ)w+(ρ)dwAˉ1(w)+w(ρ)w+(ρ)dwAˉ2(w).T=T(\rho)=\int_{w_{-}(\rho)}^{w_{+}(\rho)}\frac{dw}{|\bar A_1(w)|}+\int_{w_{-}(\rho)}^{w_{+}(\rho)}\frac{dw}{|\bar A_2(w)|}.

This describes the proposed nearly periodic behavior of the slowest variable in the deterministic fully coupled averaging regime; the statement is presented as a conjectural prediction, and no resolution is supplied in the source.

Sources & referencesView supporting material

Primary source

Yuri Kifer, “Large deviations and adiabatic transitions for dynamical systems and Markov processes in fully coupled averaging”, arXiv:0710.2405 (2007).

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