20 research outputs found

    Distinct high-T transitions in underdoped Ba1−x_{1-x}Kx_{x}Fe2_{2}As2_{2}

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    In contrast to the simultaneous structural and magnetic first order phase transition T0T_{0} previously reported, our detailed investigation on an underdoped Ba0.84_{0.84}K0.16_{0.16}Fe2_{2}As2_{2} single crystal unambiguously revealed that the transitions are not concomitant. The tetragonal (τ\tau: I4/mmm) - orthorhombic (ϑ\vartheta: Fmmm) structural transition occurs at TS≃T_{S}\simeq 110 K, followed by an adjacent antiferromagnetic (AFM) transition at TN≃T_{N}\simeq 102 K. Hysteresis and coexistence of the τ\tau and ϑ\vartheta phases over a finite temperature range observed in our NMR experiments confirm the first order character of the structural transition and provide evidence that both TST_{S} and TNT_{N} are strongly correlated. Our data also show that superconductivity (SC) develops in the ϑ\vartheta phase below TcT_{c} = 20 K and coexists with long range AFM. This new observation, TS≠TNT_{S}\neq T_{N}, firmly establishes another similarity between the hole-doped BaFe2_{2}As2_{2} via K substitution and the electron-doped iron-arsenide superconductors.Comment: 4 pages, 3 figure

    Compensation temperatures and exchange bias in La1.5Ca0.5CoIrO6

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    We report on the study of magnetic properties of the La1.5Ca0.5CoIrO6 double perovskite. Via ac magnetic susceptibility we have observed evidence of weak ferromagnetism and reentrant spin glass behavior on an antiferromagnetic matrix. Regarding the magnetic behavior as a function of temperature, we have found that the material displays up to three inversions of its magnetization, depending on the appropriate choice of the applied magnetic field. At low temperature the material exhibit exchange bias effect when it is cooled in the presence of a magnetic field. Also, our results indicate that this effect may be observed even when the system is cooled at zero field. Supported by other measurements and also by electronic structure calculations, we discuss the magnetic reversals and spontaneous exchange bias effect in terms of magnetic phase separation and magnetic frustration of Ir4+ ions located between the antiferromagnetically coupled Co ions.Comment: 10 pages, 8 figures and supplemental materia

    Pressure and chemical substitution effects in the local atomic structure of BaFe2As2

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    The effects of K and Co substitutions and quasi-hydrostatic applied pressure (P<9 GPa) in the local atomic structure of BaFe2As2, Ba(Fe{0.937}Co{0.063})2As2 and Ba{0.85}K{0.15}Fe2As2 superconductors were investigated by extended x-ray absorption fine structure (EXAFS) measurements in the As K absorption edge. The As-Fe bond length is found to be slightly reduced (<~ 0.01 Angstroms) by both Co and K substitutions, without any observable increment in the corresponding Debye Waller factor. Also, this bond is shown to be compressible (k = 3.3(3)x10^{-3} GPa^{-1}). The observed contractions of As-Fe bond under pressure and chemical substitutions are likely related with a reduction of the local Fe magnetic moments, and should be an important tuning parameter in the phase diagrams of the Fe-based superconductors.Comment: 7 pages, 6 figure

    Absence of zero-field-cooled exchange bias effect in single crystalline La2−xAx CoMnO6 (A=Ca,Sr) compounds

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    Magnetic properties of A2BB'O6 (A = rare or alkaline-earth ions; B, B' = transition-metal ions) double perovskites are of great interest due to their potential spintronic applications. Particularly fascinating is the zero-field-cooled exchange bias effect observed for the hole-doped La2−xAxCoMnO6 polycrystalline samples. In this paper we synthesize La2CoMnO6, La1.5Ca0.5CoMnO6, and La1.5Sr0.5CoMnO6 single crystals by the floating zone method and study their magnetic behavior. The three materials are ferromagnetic. Surprisingly, we observe no zero or even conventional exchange bias effect for the Ca- and Sr-doped single crystals, in sharp contrast to polycrystalline samples. This absence indicates that the lack of grain boundaries and spin-glass-like behavior, not observed in our samples, might be key ingredients for the spontaneous exchange bias phenomena seen in polycrystalline samples

    data for &quot;A phenomenological model for the spontaneous exchange bias effect&quot;

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    these data will be published in the &quot;A phenomenological model for the spontaneous exchange bias effect&quot; articleTHIS DATASET IS ARCHIVED AT DANS/EASY, BUT NOT ACCESSIBLE HERE. TO VIEW A LIST OF FILES AND ACCESS THE FILES IN THIS DATASET CLICK ON THE DOI-LINK ABOV

    The spontaneous exchange bias effect in La2-xCaxCoMnO6 series

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    Structural, electronic and magnetic properties of polycrystalline La2-xCaxCoMnO6 (0 ≤\leq x ≤\leq 0.75) compounds are investigated by x-ray diffraction and magnetometry. All the samples have an orthorhombic structure and show a slight decrease in the unit cell with Ca-doping. Temperature-dependent magnetization measurements reveal a complex magnetic behavior with two ferromagnetic transitions. These transitions are ascribed to Co2+--Mn4+ and Co3+--Mn3+ couplings and suggest the presence of additional antiferromagnetic couplings in these disordered compounds. Field-dependent magnetization curves, measured after cooling the samples in a zero external magnetic field, reveal the spontaneous exchange bias (SEB) effect for the Ca-doped samples. The strengthening of the uncompensated magnetic coupling at the interfaces, caused by the increased antiferromagnetic phase, explains the increase of SEB with increasing the Ca-content.Comment: 16 pages, 4 figure
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