A dynamic mean-field model for first-order phase transitions exhibits several hysteresis scaling universality classes governed by distinct fixed points depending on driving rate and noise presence.
This is to change every quantity O to O′ through O = O′b− [O] for a scaling factor b, where we have utilized the square brackets to denote the scale dimension
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Fixed points and crossovers for the hysteresis scaling of dynamic mean-field models
A dynamic mean-field model for first-order phase transitions exhibits several hysteresis scaling universality classes governed by distinct fixed points depending on driving rate and noise presence.