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We consider the long-range random field Ising model in dimension , whereas the long-range interaction is of the form with for and with for . Our main results establish phase transitions in these regimes. In one dimension, we employ a Peierls argument with some novel modification, suitable for dealing with the randomness coming from the external field; in two dimensions, our proof follows that of Affonso, Bissacot, and Maia (2023) with some adaptations, but new ideas are required in the critical case of .

生成讲解博客的中文版本

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