Abstract

Two numerical strategies based on the Wang–Landau and Lee entropic sampling schemesare implemented to investigate the first-order transition features of the 3D bimodal(± h)random-field Ising model at the strong disorder regime. We consider simple cubic lattices with linear sizes inthe range L = 4–32 and simulate the system for two values of the disorder strength:h = 2 and 2.25. The nature of the transition is elucidated by applying the Lee–Kosterlitz free-energybarrier method. Our results indicate that, despite the strong first-order-like characteristics,the transition remains continuous, in disagreement with the early mean-field theoryprediction of a tricritical point at high values of the random field.

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