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We have developed a Langevin dynamic simulation of high speed switching in longitudinal thin-film media. The model assumes a randomly placed set of grains with a particle size distribution which interact via magnetostatic and exchange fields. The dynamic properties of the material are simulated using the Langevin dynamic formalism which is essentially the Landau–Lifshitz–Gilbert equation of motion augmented by a random field whose properties are determined by the fluctuation–dissipation theorem. We have simulated pulsed-field magnetization and remanence curves which are obtained by applying a field pulse to a system in the remanent magnetization state. Calculations of the time dependence of the magnetization, and the time dependence of the coercivity have been made. The high frequency dynamic behavior of the systems is found to be strongly dependent on the value of the exchange coupling between the grains.
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Hannay et al. (1999) studied this question.
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