Skorokhod, Anatoli V. Quasistable gradient and Hamiltonian systems with a pairwise interaction randomly perturbed by Wiener processes. (English) Zbl 1027.60061 J. Appl. Math. Stochastic Anal. 16, No. 1, 45-67 (2003). Let \(w_k\) be a sequence of independent standard Wiener processes in \(R^d\), \(x_k\) be a finite or infinite sequence of \(R^d\)-valued stochastic processes that describe the evolution of a set of randomly perturbed pairwise interacting particles. Gradient and Hamiltonian systems of the form \[ dx_k(t)=F_k(t) dt+\sigma dw_k(t) \quad\text{and}\quad d\dot{x}_k(t)=F_k(t) dt+ \sigma dw_k(t), \] respectively, are considered, where \(F_k=-\sum_{j\neq k}U_k(x_k(t)-x_j(t))\). The assumptions on the potential \(U\) and on initial conditions, sufficient for the quasistability of both the systems, are established. Here quasistability means that any joint distributions of corresponding finite \(N\)-particle systems have a limit as \(N\rightarrow\infty\). The main assumptions include the existence of gradient (Hamiltonian) free particle system, the relation \(\lim_{s\downarrow 0}s^{\alpha+1}u''(s)=a\) for \(\alpha<1\), and some estimates for the initial configuration. Reviewer: Yuliya S.Mishura (Kyïv) Cited in 2 Documents MSC: 60H10 Stochastic ordinary differential equations (aspects of stochastic analysis) 60H30 Applications of stochastic analysis (to PDEs, etc.) 34F05 Ordinary differential equations and systems with randomness 37Jxx Dynamical aspects of finite-dimensional Hamiltonian and Lagrangian systems 60G46 Martingales and classical analysis 60K35 Interacting random processes; statistical mechanics type models; percolation theory Keywords:gradient and Hamiltonian systems; Wiener process; quasistability PDF BibTeX XML Cite \textit{A. V. Skorokhod}, J. Appl. Math. Stochastic Anal. 16, No. 1, 45--67 (2003; Zbl 1027.60061) Full Text: DOI EuDML