Pressure–temperature phase diagram of the heavy-electron superconductor [formula omitted

Abstract

The pressure–temperature phase diagram of the heavy-electron superconductor URu 2 Si 2 has been reinvestigated by AC-susceptibility and elastic neutron-scattering (NS) measurements performed on a small single-crystalline rod ( 2 mm in diameter, 6 mm in length) in a Cu–Be clamp-type high-pressure cell ( P < 1.1 GPa ) . At ambient pressure, this sample shows the weakest antiferromagnetic (AF) Bragg reflections reported so far, corresponding to the volume-averaged staggered moment of μ o ∼ 0.011 μ B / U . Under applied pressure, the AF scattering intensity exhibits a sharp increase at P ∼ 0.7 GPa at low temperatures. The saturation value of the AF scattering intensity above 0.7 GPa corresponds to μ o ∼ 0.41 μ B / U , which is in good agreement with that ( ∼ 0.39 μ B / U ) observed above 1.5 GPa in our previous NS measurements. The superconductivity is dramatically suppressed by the evolution of AF phase, indicating that the superconducting state coexists only with the hidden order phase. The presence of parasitic ferro- and/or antiferromagnetic phases with transition temperatures T 1 ⋆ = 120 ( 5 ) , T 2 ⋆ = 36 ( 3 ) and T 3 ⋆ = 16.5 ( 5 ) K and their relationship to the low- T ordered phases are also discussed.