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.
The dynamic equation reduces to dφ/dt = − a2φ + H + ζ
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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.