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The main specifics of the theory of spin dynamics in disordered solids result from the fact that calculation of observable values muststart from the solution of the equation of motion, and then they should be averaged over random distribution of spins in the sample. Nominallyany problem in statistical physics looks analogous, but the content of existing text books contains much more simple bypass methods to achievethe results. An important bypass class, determined in the preceding century, consists of problems that are equivalent to the motion of weak (orseldom) interacting (quasi)particles in translational invariant media. The basis of this solution is formed by the Boltzmann equation (devisedin the 19th century) and by methods of deriving hydrodynamic equations based on this foundation [1]. Other important advancements in physical kinetics are connected with the invention ofa projection technique byNakajima–Zwanzig for deriving various masterequations...
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