Abstract.
We investigate, by means of extensive Monte Carlo simulations, the magnetic critical behavior of the three-dimensional bimodal random-field Ising model at the strong disorder regime. We present results in favor of the two-exponent scaling scenario, \(\bar{\eta}\) = 2η, where η and \(\bar{\eta}\) are the critical exponents describing the power-law decay of the connected and disconnected correlation functions and we illustrate, using various finite-size measures and properly defined noise to signal ratios, the strong violation of self-averaging of the model in the ordered phase.
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Fytas, N., Malakis, A. Scaling and self-averaging in the three-dimensional random-field Ising model. Eur. Phys. J. B 79, 13–20 (2011). https://doi.org/10.1140/epjb/e2010-10404-6
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DOI: https://doi.org/10.1140/epjb/e2010-10404-6