Abstract

Using combinatorial optimisation techniques we study the critical properties of the two- and the three-dimensional Ising model with uniformly distributed random antiferromagnetic couplings (1≤Ji≤2)(1 \le J_i \le 2) in the presence of a homogeneous longitudinal field, hh, at zero temperature. In finite systems of linear size, LL, we measure the average correlation function, CL(ℓ,h)C_L(\ell,h), when the sites are either on the same sub-lattice, or they belong to different sub-lattices. The phase transition, which is of first-order in the pure system, turns to mixed order in two dimensions with critical exponents 1/ν≈0.51/ν\approx 0.5 and η≈0.7η\approx 0.7. In three dimensions we obtain 1/ν≈0.71/ν\approx 0.7, which is compatible with the value of the random-field Ising model, but we cannot discriminate between second-order and mixed-order transitions.

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