Abstract
We consider the quantum Ising chain with uniformly distributed random antiferromagnetic couplings and uniformly distributed random transverse fields () in the presence of a homogeneous longitudinal field, . 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 () there is an infinite disorder quantum fixed point, while at the other end () there is a classical random first-order transition point. Close to this fixed point, for and 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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