“…Therefore, in order to maintain the defect concentration at a no damage level avoiding brittle failure of the solid, there should be a particular mechanism that balances the process of thermal activation of defects with their spontaneous self-decaying by matching a difference between numbers of stationary appearing and disappearing defects at the subthreshold level. Moreover, in this case, the defects will be associated with the stochastically fluctuating thermally-excited states of a nonequilibrium quantum system weakly coupled with its equilibrium environment [5,6]. Remarkably, the kinetic equation for populations of defect states, found as a result of stochastic averaging of the microscopic Liouville-von Neumann evolution equation for the density matrix of the whole system "system + environment + weak interaction" over fast fluctuations in the states energies, being generally nonlinear and containing also states coherences, can nevertheless be reduced to a linear equation of the population balance only [4].…”