Self attracting diffusions on a sphere and application to a periodic case

preprint2015arXivOpen access

Abstract

This paper proves almost-sure convergence for the self-attracting diffusion on the unit sphere dX(t)=σdWt(X(t))−a∫0t∇SnVXs(Xt)dsdt,X(0)=x∈SndX(t)=σdW_{t}(X(t))-a\int_{0}^{t}\nabla_{\mathbb{S}^n}V_{X_s}(X_t) dsdt,\qquad X(0)=x\in\mathbb{S}^n %given by the stochastic differential equation: dXt=σdWt+a∫0tsin⁡(Xt−Xs)dsdt,dX_{t}=σdW_{t}+a\int_{0}^{t}\sin(X_{t}-X_{s})dsdt, where σ>0σ>0, a<0a < 0, Vy(x)=⟨x,y⟩V_y(x)=\langle x,y\rangle is the usual scalar product in Rn\mathbb{R}^n, and (Wt(.))t⩾0(W_{t}(.))_{t\geqslant 0} is a Brownian motion on Sn\mathbb{S}^n. From this follows the almost-sure convergence of the real-valued self-attracting diffusion dϑt=σdWt+a∫0tsin⁡(ϑt−ϑs)dsdt,d\vartheta_{t}=σdW_{t}+a\int_{0}^{t}\sin(\vartheta_{t}-\vartheta_{s})dsdt, where (Wt)t⩾0(W_t)_{t\geqslant 0} is a real Brownian motion.

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