Nearly periodic slow motion in deterministic fully coupled averaging

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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)=w∗w_{-}(\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 δ→0\delta\to0 and ε→0\varepsilon\to0 so that

lim⁡ε,δ→0εln⁡(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), t≥0t\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)dw∣Aˉ1(w)∣+∫w−(ρ)w+(ρ)dw∣Aˉ2(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.

References

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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