We study the far-from-equilibrium properties of quenched magnetic nanoscopic classical spin systems. In particular, we focus on the interplay between lattice vibrations and magnetic frustrations induced by surface effects typical of an antiferromagnet. We use a combination of Monte Carlo simulations and explore the dynamical behaviours by solving the stochastic Landau-Lifshitz-Gilbert equation at finite temperature. The Monte Carlo approach treats both the ionic degrees of freedom and spin variables on the same footing, via an extended Lennard-Jones Hamiltonian with a spinlattice coupling. The zero temperature phase diagram of the finite size nanoscopic systems with respect to the range of the Heisenberg interaction and the Lennard-Jones coupling constant shows two main structures with non-trivial magnetisation triggered by antiferromagnetism: a simple cubic and a body-centred cubic. At non zero temperature, the competition between spins and the ionic vibrations considerably affects the magnetization of the system. Exploring the dynamics reveals a non-trivial structural induced behaviour in the spin relaxation with a concomitant memory of the initially applied ferromagnetic quench. We report the observation of a non-trivial dynamical scenario, obtained after a ferromagnetic magnetic quench at low temperature. Furthermore, we observe long-lived non-thermal states which could open new avenues for nano-technology.Many-body systems comprise a wide range of systems, from simple metals, organic molecules, all the way up to cells. While their physics can be extremely rich, this complexity is however often irrelevant, as such systems will typically -at equilibrium -thermalise, a process through which most information about their preparation history and their initial state is lost [1,2]. This behaviour is typical for ergodic systems in the thermodynamic limit and allows to calculate physical observables and make predictions that can be measured and tested. However, ergodicity can be broken out-of-equilibrium [3], in particular by inducing non-thermal states that keep a memory of their initial condition for long times. Those peculiar behaviours have been explored in novel nonequilibrium phases of matter, which includes Floquet symmetry protected topological phases [4] and time crystals [5,6]. While bulk systems have been extensively investigated, nanoscopic systems remain open to questions. Recent progress in nano-engineering and the design of nanoscopic systems, such as nano-magnets made of single atoms arrays as memory devices [7], has opened new possibilities to explore quantum states in systems where thermalisation is not obtained, in particular for quenched and periodically-driven systems. Indeed, it has been observed that finite size effects allow these systems to keep a much better local memory of their initial conditions [8]. Experimental advances in manipulation and switching of the magnetization -possible even at the femtosecond level [9]-have triggered new studies in spin dynamics towards the microscopic underst...