Abstract
In this work, in the framework of the Ginzburg-Landau phenomenological theory for phase transitions it was found that the structure of the main state of a nanoscale ferroelastic plate below the phase transition temperature can be heterogeneous and is “domain-like.” By the numerical solution of a nonlinear system of differential equations for the order parameter in the framework of elasticity theory, it is shown that in the low-temperature phase of a mechanically fixed ferroelastic plate with a size starting from a certain thickness (), an inhomogeneous domain-like state is realized. “Domains” do not have clear boundaries, but have a various signs of the order parameter, and their number depends on the proximity of the temperature to the phase transition temperature and the plate thickness.