Magnetic properties of NpPd3and PuPd3intermetallic compounds

Abstract
Magnetization, electrical-resistivity, Mössbauer-effect, and neutron-diffraction measurements have been made between 1.5 and 300 °K for two phases of NpPd3 and for PuPd3. The compounds PuPd3 and cubic NpPd3 have the AuCu3-type crystal structure. Hexagonal NpPd3 has the TiNi3-type structure and is the room-temperature equilibrium phase. Cubic NpPd3 can be retained by rapid quenching, and the specimen used in this investigation has a long-range order parameter of S=0.92. The cubic NpPd3 compound is antiferromagnetic with a Néel temperature TN=(55±1) °K, and the magnetic transition is apparently first order, since the sublattice magnetization is constant up to 45 °K. A large energy gap Δ in the spin-wave dispersion relation is observed below 40 °K in the electrical resistivity with Δ3kTNkΘk(150 °K), where Θ is the Debye temperature obtained from the resistivity data. Cubic PuPd3 is antiferromagnetic below 24 °K. Cubic NpPd3 and PuPd3 have a magnetic structure that consists of ferromagnetic (111) planes coupled antiferromagnetically, and they have ordered moments of (2.0±0.1) μB/Np atom and (0.8±0.1) μB/Pu atom, respectively. Hexagonal NpPd3 does not possess long-range magnetic order, but does appear to have an abrupt transition to short-range magnetic order distributed throughout the bulk below ∼32 °K, as indicated by an apparent Curie temperature in the magnetization, a spin-disorder resistivity anomaly, and a broadening of the paramagnetic Mössbauer line as the temperature is lowered from 30 to 4.2 °K. Both NpPd3 phases have the same effective paramagnetic moment of 2.74 μB/Np atom, consistent with the Np3+ ionic configuration, the same volume per formula unit, and essentially the same first-and second-nearest-neighbor neptunium environment. The difference in magnetic behavior between the cubic and hexagonal phases of NpPd3 is at present not understood.