Abstract
Relaxation phenomena in magnetic materials cover a wide range of processes in which a new equilibrium state is reached after a change of the magnetic field. The relaxation effect is due to the exchange of energy between the spins and other degrees of freedom of the system. The process is usually characterized by its relaxation time τ, in which magnetization M z will reach the equilibrium value M 0 after a change of the magnetic field from H to H + ΔH, as follows:
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Bałanda, M., von Nidda, HA.K., Heinrich, M., Loidl, A. (2003). Dynamic Susceptibility of Magnetic Systems. In: Haase, W., Wróbel, S. (eds) Relaxation Phenomena. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-09747-2_3
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