16 research outputs found

    Honeycomb lattice iridate on the verge of Mott-collapse

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    A new honeycomb lattice iridate (La,Na)IrO3_3 (β‰ˆ\approx LaNaIr2_2O6_6) is successfully synthesized from the spin-orbit coupled Mott insulator Na2_2IrO3_3 by replacing the interlayer Na+^+ ions with La3+^{3+} ions. (La,Na)IrO3_3 shows a finite Sommerfeld term in heat capacity and a βˆ’ln⁑T-\ln T dependence of resistivity, indicating a realization of a metallic state driven by a Mott collapse. Furthermore, crystal structure analysis reveals the formation of Ir zig-zag chains with metal-metal bonding, increasing kinetic energy resulting in the Mott collapse. This observation would be due to a Mott collapse induced in a Jeff=1/2J_{\mathrm{eff}} = 1/2 spin-orbit coupling Mott insulator with an Ir honeycomb lattice by topochemical control of the ionic configuration.Comment: 7pages, 5 figures, accepted in Journal of Physics: Condensed Matte

    Monoclinic distortion in hyperhoneycomb Kitaev material Ξ²\beta-ZnIrO3_3 revealed by improved sample quality

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    The sample quality of the hyperhoneycomb lattice Kitaev magnet Ξ²\beta-ZnIrO3_3 was successfully improved by removing the maximum amount of moisture from the reaction ampoule. The X-ray diffraction structural analysis of the high-quality sample confirmed the presence of PP21_1/cc superlattice peaks of the Fddd structure in the original structural model. These peaks could not be distinguished due to the presence of impurities in the low-quality sample in a previous study. The structural analysis based on this monoclinic crystal structure model showed no chemical disorder, suggesting that the observed spin liquid type behavior is an intrinsic property unrelated to bond randomness. The details of the Ξ²\beta-ZnIrO3_3 structure revealed in this study will stimulate the further investigation of Kitaev physics.Comment: 4pages, 3figure

    Magnetic ordering in the JeffJ_{\rm eff} = 0 Nickelate NiRh2_2O4_4 prepared via a solid-state metathesis

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    In spinel-type nickelate NiRh2_2O4_4, magnetic ordering is observed upon the sample synthesized via kinetically controlled low-temperature solid-state metathesis, as opposed to previously-reported samples obtained through conventional solid-state reaction. Our findings are based on a combination of bulk susceptibility and specific heat measurements that disclose a Neˊ\'eel transition temperature of TNT_N = 45 K in this material, which might feature spin-orbit entanglement in the tetragonally-coordinated d8d^8 Mott insulators. The emergence of magnetic ordering upon alteration of the synthesis route indicates that the suppression of magnetic ordering in the previous sample was rooted in the cation-mixing assisted by the entropy gain that results from high-temperature reactions. Furthermore, the JeffJ_{\rm eff} = 0 physics, instead of solely the spin-only S=1S = 1, describes the observed enhancement of effective magnetic moment well. Overseeing all observations and speculations, we propose that the possible mechanism responsible for the emergent magnetic orderings in NiRh2_2O4_4 is the condensation of JeffJ_{\rm eff} = 0 exciton, driven by the interplay of the tetragonal crystal field and superexchange interactions.Comment: 7 pages, 5 figures, accepted in Physical Review Material

    Magnetic Phase Transition and Magnetization Plateau in Cs2_2CuBr4_4

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    The crystal structure of Cs2_2CuBr4_4 is the same as that of Cs2_2CuCl4_4, which has been characterized as a spin-1/2 quasi-two-dimensional frustrated system. The magnetic properties of Cs2_2CuBr4_4 were investigated by magnetization and specific heat measurements. The phase transition at zero magnetic field was detected at TN=1.4T_{\rm N}=1.4 K. It was observed that the magnetization curve has a plateau at about one-third of the saturation magnetization for magnetic field HH parallel to the bb- and cc-axes, while no plateau was observed for Hβˆ₯aH\parallel a. The field-induced phase transition to the plateau state appears to be of the first order. The mechanism leading to the magnetization plateau is discussed.Comment: 6 pages, 4 figures, 4 eps files, ptptex, will appear in Supplement of Progress in Theoretical Physic

    Perfect kagome-lattice antiferromagnets with Jeff_{eff} = 1/2: The Co2+^{2+}-analogs of copper minerals volborthite and vesignieite

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    We report the synthesis, crystal structure, and magnetic properties of Co2+^{2+} kagome magnets Co3_3V2_2O7_7(OH)2_2β‹…\cdot2H2_2O and BaCo3_3(VO4_4)2_2(OH)2_2, which can be recognized as Co-analogues of the intensively researched quantum kagome magnet volborthite Cu3_3V2_2O7_7(OH)2_2β‹…\cdot2H2_2O and vesignieite BaCu3_3(VO4_4)2_2(OH)2_2. For each compound, the ground state is seemingly A-type antiferromagnetic order. At low temperatures, applying a magnetic field causes a metamagnetic-like transition described by the transition in which antiferromagnetically-aligned canted moments change to ferromagnetically-aligned ones. These ground and field-induced states include a canted ferromagnetic component perpendicular to the kagome planes favored by Dzyaloshinskii-Moriya interactions. These magnetic properties are well characterized by the Jeff_{eff} = 1/2 physics. Our findings will be the first step toward clarifying the Jeff_{eff} = 1/2 kagome physics, which has been little studied experimentally or theoretically.Comment: 9 pages, 7+1 figures, accepted for publication in Physical Review

    Isothermal remanent magnetization and the spin dimensionality of spin glasses

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    The isothermal remanent magnetization is used to investigate dynamical magnetic properties of spatially three dimensional spin glasses with different spin dimensionality (Ising, XY, Heisenberg). The isothermal remanent magnetization is recorded vs. temperature after intermittent application of a weak magnetic field at a constant temperature ThT_h. We observe that in the case of the Heisenberg spin glasses, the equilibrated spin structure and the direction of the excess moment are recovered at ThT_h. The isothermal remanent magnetization thus reflects the directional character of the Dzyaloshinsky-Moriya interaction present in Heisenberg systems.Comment: tPHL2e style; 7 page, 3 figure
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