Magnetic and transport properties ofPb1xMnxTespin-glass

Abstract
Magnetic properties of Pb1xMnxTe are reported for Mn concentrations x0.2. Below 1 K, a spin-glass behavior is observed, characterized by a thermoremanent magnetization which has been studied as a function of time and of the magnetic field. The freezing temperature Tg defined by a cusp in the reversible part of the magnetic susceptibility is found to be associated with the occurrence of a spin-glass state rather than a clustering effect as in the other manganese compound Cd1xMnxTe. We attribute this result to the existence of long-range interband exchange interactions arising from the fact that Pb1xMnxTe is a small-gap semiconductor. For all Mn concentrations, antiferromagnetic interactions are shown to dominate, in opposition with previous theoretical predictions. Above Tg, the material is in a superparamagnetic state due to short-range antiferromagnetic superexchange interactions. It is shown that a mean-field approximation accounts very well for the experimental results, above a temperature TM2Tg up to a magnetic field H10 kG, but breaks down at T<TM. This effect is related to the pathological behavior of the functional dependence of the magnetization on the magnetic field above the de Almeida—Thouless instability temperature. All the samples were p type. The transport experiments show that the valence band is significantly perturbed upon introduction of Mn in the matrix. In particular, a crossing between valleys of the valence band with extrema at the L points of the Brillouin zone and the valleys with extrema along the Σ (symmetry) directions, is inferred at x0.114 at low temperatures. At high magnetic field, the magnetoresistance associated with the diffusion of holes by the spin fluctuations is shown to be positive, although a negative magnetoresistance can be observed in the low-field limit on some samples.