Abstract
We consider the random transverse-field Ising model in dimensions with long-range ferromagnetic interactions which decay as a power with the distance. Using a variant of the strong disorder renormalization group method we study numerically the phase-transition point from the paramagnetic side. The distribution of the (sample dependent) pseudo-critical points is found to scale with , being the linear size of the sample. Similarly, the critical magnetization scales with and the excitation energy behaves as . Using extreme-value statistics we argue that extrapolating from the ferromagnetic side the magnetization approaches a finite limiting value and thus the transition is of mixed-order.
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