A nonlinear phenomenological model of magnetic dissipation is proposed. This model is a generalization of a standard Gilbert model, where the constant Gilbert damping parameter αG is replaced by a function αG(ξ) of the dimensionless scalar quantity ξ proportional to the square of the time rate of change of the magnetization vector (∂M∕∂t)². The proposed model is illustrated for the example of magnetization precession excited by spin-polarized current in an in-plane magnetized nanopillar---the case where the standard Gilbert model leads to qualitatively incorrect results that contradict experiments.
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Tiberkevich et al. (2007) studied this question.
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