67 research outputs found

    Stabilization of the high-spin state of Co3+^{3+} in LaCo1x_{1-x}Rhx_{x}O3_3

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    The rhodium doping in the LaCo1x_{1-x}Rhx_{x}O3_3 perovskite series (x=0.020.5x=0.02-0.5) has been studied by X-ray diffraction, electric transport and magnetization measurements, complemented by electronic structure GGA+U calculations in supercell for different concentration regimes. No charge transfer between Co3+^{3+} and Rh3+^{3+} is evidenced. The diamagnetic ground state of LaCoO3_3, based on Co3+^{3+} in low-spin (LS) state, is disturbed even by a small doping of Rh. The driving force is the elastic energy connected with incorporation of a large Rh3+^{3+} cation into the matrix of small LS Co3+^{3+} cations, which is relaxed by formation of large Co3+^{3+} in high-spin (HS) state in the next-nearest sites to the inserted Rh atom. With increasing temperature, the population of Co3+^{3+} in HS state increases through thermal excitation, and a saturated phase is obtained close to room temperature, consisting of a nearest-neighbor correlation of small (LS Co3+^{3+}) and large (HS Co3+^{3+} and LS Rh3+^{3+}) cations in a kind of double perovskite structure. The stabilizing role of elastic and electronic energy contributions is demonstrated in supercell calculations for dilute Rh concentration compared to other dopants with various trivalent ionic radius.Comment: 8 pages, 8 figure

    Metal-insulator transition and the Pr3+^{3+}/Pr4+^{4+} valence shift in (Pr1y_{1-y}Yy_{y})0.7_{0.7}Ca0.3_{0.3}CoO3_3

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    The magnetic, electric and thermal properties of the (Ln1yLn_{1-y}Yy_{y})0.7_{0.7}Ca0.3_{0.3}CoO3_3 perovskites (LnLn~=~Pr, Nd) were investigated down to very low temperatures. The main attention was given to a peculiar metal-insulator transition, which is observed in the praseodymium based samples with y=0.075y=0.075 and 0.15 at TMI=64T_{M-I}=64 and 132~K, respectively. The study suggests that the transition, reported originally in Pr0.5_{0.5}Ca0.5_{0.5}CoO3_3, is not due to a mere change of cobalt ions from the intermediate- to the low-spin states, but is associated also with a significant electron transfer between Pr3+^{3+} and Co3+^{3+}/Co4+^{4+} sites, so that the praseodymium ions occur below TMIT_{M-I} in a mixed Pr3+^{3+}/Pr4+^{4+} valence. The presence of Pr4+^{4+} ions in the insulating phase of the yttrium doped samples (Pr1y_{1-y}Yy_{y})0.7_{0.7}Ca0.3_{0.3}CoO3_3 is evidenced by Schottky peak originating in Zeeman splitting of the ground state Kramers doublet. The peak is absent in pure Pr0.7_{0.7}Ca0.3_{0.3}CoO3_3 in which metallic phase, based solely on non-Kramers Pr3+^{3+} ions, is retained down to the lowest temperature.Comment: 10 figure

    Magnetodielectric effect and optic soft mode behaviour in quantum paraelectric EuTiO3 ceramics

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    Infrared reflectivity and time-domain terahertz transmission spectra of EuTiO3 ceramics revealed a polar optic phonon at 6 - 300K, whose softening is fully responsible for the recently observed quantum paraelectric behaviour. Even if our EuTiO3 ceramics show lower permittivity than the single crystal due to a reduced density and/or small amount of secondary pyrochlore Eu2Ti2O7 phase, we confirmed the magnetic field dependence of the permittivity, also slightly smaller than in single crystal. Attempt to reveal the soft phonon dependence at 1.8K on the magnetic field up to 13T remained below the accuracy of our infrared reflectivity experiment

    Synchronization of multi-phase oscillators: An Axelrod-inspired model

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    Inspired by Axelrod's model of culture dissemination, we introduce and analyze a model for a population of coupled oscillators where different levels of synchronization can be assimilated to different degrees of cultural organization. The state of each oscillator is represented by a set of phases, and the interaction --which occurs between homologous phases-- is weighted by a decreasing function of the distance between individual states. Both ordered arrays and random networks are considered. We find that the transition between synchronization and incoherent behaviour is mediated by a clustering regime with rich organizational structure, where some of the phases of a given oscillator can be synchronized to a certain cluster, while its other phases are synchronized to different clusters.Comment: 6 pages, 5 figure

    Hole-doping dependence of percolative phase separation in Pr_(0.5-delta)Ca_(0.2+delta)Sr_(0.3)MnO_(3) around half doping

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    We address the problem of the percolative phase separation in polycrystalline samples of Pr0.5δ_{0.5-\delta}Ca0.2+δ_{0.2+\delta}Sr0.3_{0.3}MnO3_3 for 0.04δ0.04-0.04\leq \delta \leq 0.04 (hole doping nn between 0.46 and 0.54). We perform measurements of X-ray diffraction, dc magnetization, ESR, and electrical resistivity. These samples show at TCT_C a paramagnetic (PM) to ferromagnetic (FM) transition, however, we found that for n>0.50n>0.50 there is a coexistence of both of these phases below TCT_C. On lowering TT below the charge-ordering (CO) temperature TCOT_{CO} all the samples exhibit a coexistence between the FM metallic and CO (antiferromagnetic) phases. In the whole TT range the FM phase fraction (XX) decreases with increasing nn. Furthermore, we show that only for n0.50n\leq 0.50 the metallic fraction is above the critical percolation threshold XC15.5X_C\simeq 15.5%. As a consequence, these samples show very different magnetoresistance properties. In addition, for n0.50n\leq 0.50 we observe a percolative metal-insulator transition at TMIT_{MI}, and for TMI<T<TCOT_{MI}<T<T_{CO} the insulating-like behavior generated by the enlargement of XX with increasing TT is well described by the percolation law ρ1=σ(XXC)t\rho ^{-1}=\sigma \sim (X-X_C)^t, where tt is a critical exponent. On the basis of the values obtained for this exponent we discuss different possible percolation mechanisms, and suggest that a more deep understanding of geometric and dimensionality effects is needed in phase separated manganites. We present a complete TT vs nn phase diagram showing the magnetic and electric properties of the studied compound around half doping.Comment: 9 text pages + 12 figures, submitted to Phys. Rev.

    First-principles design and subsequent synthesis of a material to search for the permanent electric dipole moment of the electron

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    We describe the first-principles design and subsequent synthesis of a new material with the specific functionalities required for a solid-state-based search for the permanent electric dipole moment of the electron. We show computationally that perovskite-structure europium barium titanate should exhibit the required large and pressure-dependent ferroelectric polarization, local magnetic moments, and absence of magnetic ordering even at liquid helium temperature. Subsequent synthesis and characterization of Eu0.5_{0.5}Ba0.5_{0.5}TiO3_3 ceramics confirm the predicted desirable properties.Comment: Nature Materials, in pres
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