Limiting Behavior of Non-Autonomous Stochastic Reversible Selkov Lattice Systems Driven by Locally Lipschitz Lévy Noises

This work investigates the long-term distributional behavior of the reversible Selkov lattice systems defined on the set $\mathbb{Z}$ and driven by locally Lipschitz \emph{Lévy noises}, which possess two pairs of oppositely signed nonlinear terms and whose nonlinear couplings can grow polynomially with any order $p\ge 1$. Firstly, based on the global-in-time well-posedness in $L^2(\mathrm{\Omega },{\mathrm{\ell }}^2\times {\mathrm{\ell }}^2)$, we define a \emph{continuous} non-autonomous dynamical system (NDS) on the metric space $({\mathcal{P}}_2({\mathrm{\ell }}^2\times {\mathrm{\ell }}^2),d_{\mathcal{P}({\mathrm{\ell }}^2\times {\mathrm{\ell }}^2)})$, where $d_{\mathcal{P}({\mathrm{\ell }}^2\times {\mathrm{\ell }}^2)}$ is the dual-Lipschitz distance on $\mathcal{P}({\mathrm{\ell }}^2\times {\mathrm{\ell }}^2)$, the space of probability measures on ${\mathrm{\ell }}^2\times {\mathrm{\ell }}^2$. Specifically, we establish that this non-autonomous dynamical system admits a unique pullback measure attractor, characterized via measure-valued complete solutions and orbits in the sense of Wang (DOI.org/10.1016/j.jde.2012.05.015). Moreover, when the deterministic external forcing terms are periodic in time, we demonstrate that the pullback measure attractors are also periodic. We also study the upper semicontinuity of pullback measure attractors as $({\epsilon }_1,{\epsilon }_2,{\gamma }_1,{\gamma }_2)\to (0,0,0,0)$. The main difficulty in proving the pullback asymptotic compactness of the NDS in $({\mathcal{P}}_2({\mathrm{\ell }}^2\times {\mathrm{\ell }}^2),d_{\mathcal{P}({\mathrm{\ell }}^2\times {\mathrm{\ell }}^2)})$ is caused by the lack of compactness in infinite-dimensional lattice systems, which is overcome by using uniform tail-ends estimates. And the inherent structure of the Selkov system precludes the possibility of any unidirectional dissipative influence arising from the interaction between the two coupled equations, thereby obstructing the emergence of a dominant energy-dissipation mechanism along a single directional pathway.