Abstract

We consider the quantum Ising chain with uniformly distributed random antiferromagnetic couplings (1≤Ji≤2)(1 \le J_i \le 2) and uniformly distributed random transverse fields (Γ0≤Γi≤2Γ0Γ_0 \le Γ_i \le 2Γ_0) in the presence of a homogeneous longitudinal field, hh. Using different numerical techniques (DMRG, combinatorial optimisation and strong disorder RG methods) we explore the phase diagram, which consists of an ordered and a disordered phase. At one end of the transition line (h=0,Γ0=1h=0,Γ_0=1) there is an infinite disorder quantum fixed point, while at the other end (h=2,Γ0=0h=2,Γ_0=0) there is a classical random first-order transition point. Close to this fixed point, for h>2h>2 and Γ0>0Γ_0>0 there is a reentrant ordered phase, which is the result of quantum fluctuations by means of an order through disorder phenomenon.

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