Hysteresis loops are often observed in experiments in first order phase transformations when the system goes out of equilibrium. They may have a macroscopic jump, roughly as seen in the supercooling of liquids, or they may be smoothly varying, as seen in most magnets. The nonequilibrium zero-temperature random-field Ising-model can be used to model hysteretic behavior in first order phase transformations: as the disorder is decreased, one finds a transition from smooth hysteresis loops to loops with a sharp jump in magnetization (corresponding to an infinite avalanche). In a large region near the transition point the model exhibits power law distributions of noise (avalanches), universal behavior and a diverging length scale. Universal properties of this critical point are reported that were obtained using renormalization group methods and numerical simulations. Connections to experimental systems such as athermal martensitic phase transitions (with and without "bursts") and the Barkhausen effect in magnetic systems are discussed.
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Dahmen et al. (2000) studied this question.
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