The rich phase diagrams of magnetically frustrated pyrochlores have maintained a high level of interest over the past 20 years. To experimentally explore these phase diagrams requires a means of tuning the relevant interactions. One approach to achieve this is chemical pressure, that is, varying the size of the non-magnetic cation. Here, we report on a new family of lead-based pyrochlores A2Pb2O7 (A = Pr, Nd, Gd), which we have characterized with magnetic susceptibility and specific heat. Lead is the largest known possible B-site cation for the pyrochlore lattice. Thus, these materials significantly expand the phase space of the frustrated pyrochlores. Pr2Pb2O7 has an absence of long-range magnetic order down to 400 mK and a spin ice-like heat capacity anomaly at 1.2 K. Thus, Pr2Pb2O7 is a candidate for a quantum spin ice state, despite weaker exchange. Nd2Pb2O7 transitions to a magnetically ordered state at 0.41 K. The Weiss temperature for Nd2Pb2O7 is θCW = −0.06 K, indicating close competition between ferromagnetic and antiferromagnetic interactions. Gd2Pb2O7 is a Heisenberg antiferromagnet that transitions to long-range magnetic order at 0.81 K, in spite of significant site mixing. Below its ordering transition, we find a T 3/2 heat capacity dependence in Gd2Pb2O7, indication of a ground state that is distinct from other gadolinium pyrochlores. These lead-based pyrochlores provide insight into the effects of weakened exchange on highly frustrated lattices and represent further realizations of several exotic magnetic ground states which can test theoretical models.
The frustrated double perovskite La 2 LiOsO 6 , based on Os 5+ (5d 3 , t 2 3) is studied using magnetization, elastic neutron scattering, heat capacity and muon spin relaxation(μSR) techniques and compared with iso structural (P2 1 /n) La 2 LiRuO 6 , Ru 5+ (4d 3 ,t 2 3). While previous studies of La 2 LiOsO 6 showed a broad susceptibility maximum (χ max) near 40K, heat capacity data indicate a sharp peak at 30K, similar to La 2 LiRuO 6 with χ max ~ 30K and a heat capacity peak at 24K. Significant differences between the two materials are seen in powder neutron diffraction where the magnetic structure is described by k = (1/2 1/2 0) for La 2 LiOsO 6 , while La 2 LiRuO 6 has been reported with k = (000), structure for face centered lattices. For the k = (1/2 1/2 0) structure one has antiferromagnetic layers stacked antiferromagnetically, while in the Type I structure, ferromagnetic layers are stacked antiferromagnetically. In spite of these differences both can be considered as TypeI f.c.c. antiferromagnetic structures. For La 2 LiOsO 6 the magnetic structure is best described in terms of linear combinations of basis vectors belonging to irreducible representations Γ2 and Γ4. The combinations Γ2-Γ4 and Γ2 + Γ4 could not be distinguished from refinement of the data. In all cases the Os 5+ moments lie in the yz plane with the largest component along y. The total moment is 1.81(4)μ B. For La 2 LiRuO 6 the Ru 5+ moments are reported to lie in the xz plane. In addition, while neutron diffraction, μSR and NMR data indicate an unique T N = 24K for La 2 LiRuO 6 , the situation for La 2 LiOsO 6 is more complex, with heat capacity, neutron diffraction and μSR indicating two ordering events at 30K and 37K, similar to the cases of cubic Ba 2 YRuO 6 and monoclinic Sr 2 YRuO 6 .
The gadolinium pyrochlores, Gd2B2O7, are amongst the best realizations of antiferromagnetically coupled Heisenberg spins on a pyrochlore lattice. We present a magnetic characterization of Gd2Pt2O7, a unique member of this family. Magnetic susceptibility, heat capacity, and muon spin relaxation measurements show that Gd2Pt2O7 undergoes an antiferromagnetic ordering transition at TN = 1.6 K. This transition is strongly first order, as indicated by the sharpness of the heat capacity anomaly, thermal hysteresis in the magnetic susceptibility, and a non-divergent relaxation rate in µSR. The form of the heat capacity below TN suggests that the ground state is an anisotropic collinear antiferromagnet with an excitation spectrum that is gapped by 0.245(1) meV. The ordering temperature in Gd2Pt2O7, TN = 1.6 K, is a substantial 160% increase from other gadolinium pyrochlores, which have been found to order at 1 K or lower. We attribute this enhancement in TN to the B-site cation, platinum, which, despite being non-magnetic, has a filled 5d t2g orbital and an empty 5d eg orbital that can facilitate superexchange. Thus, the magnetic frustration in Gd2Pt2O7 is partially "relieved", thereby promoting magnetic order.
The crystal structure of KRuO is refined at both 280 and 3.5 K from neutron powder data, and magnetic properties are reported for the first time. The scheelite structure, I4/a, is confirmed at both temperatures. Atomic positions of greater accuracy than the original 1954 X-ray study are reported. The rare Ru ion resides in a site of distorted tetrahedral symmetry with nominal electronic configuration 4d(e). Curie-Weiss parameters are near free ion values for the effective moment and θ = -77 K, indicating dominant antiferromagnetic (AF) correlations. A broad susceptibility maximum occurs near 34 K, but long-range AF order sets in only below 22.4 K as determined by magnetization and heat capacity data. The entropy loss below 50 K is only 44% of the expected R ln 2, indicating the presence of short-range spin correlations over a wide temperature range. The Ru sublattice consists of centered, corner-sharing tetrahedra which can lead to geometric frustration if both the nearest-neighbor, J, and the next-nearest-neighbor, J, exchange constants are AF and of similar magnitude. A spin dimer analysis finds J/J ≈ 25, indicating weak frustration, and a (d) ground state. A single, weak magnetic reflection was indexed as (110). The absence of the (002) magnetic reflection places the Ru moments parallel to the c axis. The Ru moment is estimated to be 0.57(7) μ, reduced from an expected value near 1 μ. A recent computational study of isostructural, isoelectronic KOsO predicts a surprisingly large orbital moment due to spin-orbit coupling (SOC). However, the free ion SOC constant for Ru is only ∼30% that of Os, so it is unclear that this effect can be implicated in the low ordered moment for KRuO. The origin of the short-range spin correlations is also not understood.
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