4 research outputs found

    Incorporation of Jahnā€“Teller Cu<sup>2+</sup> Ions into Magnetoelectric Multiferroic MnWO<sub>4</sub>: Structural, Magnetic, and Dielectric Permittivity Properties of Mn<sub>1ā€“<i>x</i></sub>Cu<sub><i>x</i></sub>WO<sub>4</sub> (<i>x</i> ā‰¤ 0.25)

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    Polycrystalline samples of Mn<sub>1ā€“<i>x</i></sub>Cu<sub><i>x</i></sub>WO<sub>4</sub> (<i>x</i> ā‰¤ 0.5) have been prepared by a solid-state synthesis as well as from a citrate synthesis at moderate temperature (850 Ā°C). The goal is to study changes in the structural, magnetic, and dielectric properties of magnetoelectric type-II multiferroic MnWO<sub>4</sub> caused by replacing Jahnā€“Teller-inactive Mn<sup>2+</sup> (d<sup>5</sup>, <i>S</i> = 5/2) ions with Jahnā€“Teller-active Cu<sup>2+</sup> (d<sup>9</sup>, <i>S</i> = 1/2) ions. Combination of techniques including scanning electron microscopy, powder X-ray and neutron diffraction, and Raman spectroscopy demonstrates that the polycrystalline samples with low copper content 0 ā‰¤ <i>x</i> ā‰¤ 0.25 are solid solution that forms in the monoclinic <i>P</i>2/c space group. Rietveld analyses indicate that Cu atoms substitutes for Mn atoms at the Mn crystallographic site of the MnWO<sub>4</sub> structure and suggest random distributions of Jahnā€“Teller-distorted CuO<sub>6</sub> octahedra in the solid solution. Magnetic susceptibility reveals that only 5% of Cu substitution suppresses the nonpolar collinear AF1 antiferromagnetic structure observed in pure MnWO<sub>4</sub>. Type-II multiferroicity survives a weak Cu substitution rate (<i>x</i> < 0.15). Multiferroic transition temperature and NeĢel temperature increase as the amount of Cu increases. New trends in some of the magnetic properties and in dielectric behaviors are observed for <i>x</i> = 0.20 and 0.25. Careful analysis of the magnetic susceptibility reveals that the incorporation of Cu into MnWO<sub>4</sub> strengthens the overall antiferromagnetic interaction and reduces the magnetic frustration

    Pair Distribution Function and Density Functional Theory Analyses of Hydrogen Trapping by Ī³ā€‘MnO<sub>2</sub>

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    In the presence of ā€œAg<sub>2</sub>Oā€ as a promoter, Ī³-MnO<sub>2</sub> traps dihydrogen in its (2 Ɨ 1) and (1 Ɨ 1) tunnels. The course of this reaction was examined by analyzing the X-ray diffraction patterns of the H<sub><i>x</i></sub>MnO<sub>2</sub>/ā€œAg<sub>2</sub>Oā€ system (0 ā‰¤ <i>x</i> < 1) on the basis of pair distribution function and density functional theory (DFT) analyses. Hydrogen trapping occurs preferentially in the (2 Ɨ 1) tunnels of Ī³-MnO<sub>2</sub>, which is then followed by that in the (1 Ɨ 1) tunnels. Our DFT analysis shows that this process is thermodynamically favorable

    Increasing the Phase-Transition Temperatures in Spin-Frustrated Multiferroic MnWO<sub>4</sub> by Mo Doping

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    Ceramic samples of MnW<sub>1ā€“<i>x</i></sub>Mo<sub><i>x</i></sub>O<sub>4</sub> (<i>x</i> ā‰¤ 0.3) solid solution were prepared by a solid-state route with the goal of increasing the magnitude of the spin-exchange couplings among the Mn<sup>2+</sup> ions in the spin spiral multiferroic MnWO<sub>4</sub>. Samples were characterized by X-ray diffraction, optical spectroscopy, magnetization, and dielectric permittivity measurements. It was observed that the NeĢel temperature <i>T</i><sub>N</sub>, the spin spiral ordering temperature <i>T</i><sub>M2</sub>, and the ferroelectric phase-transition temperature <i>T</i><sub>FE2</sub> of MnWO<sub>4</sub> increased upon the nonmagnetic substitution of Mo<sup>6+</sup> for W<sup>6+</sup>. Like pure MnWO<sub>4</sub>, the ferroelectric critical temperature <i>T</i><sub>FE2</sub>(<i>x</i>) coincides with the magnetic ordering temperature <i>T</i><sub>M2</sub>(<i>x</i>). A density functional analysis of the spin-exchange interactions for a hypothetical MnMoO<sub>4</sub> that is isostructural with MnWO<sub>4</sub> suggests that Mo substitution increases the strength of the spin-exchange couplings among Mn<sup>2+</sup> in the vicinity of a Mo<sup>6+</sup> ion. Our study shows that the Mo-doped MnW<sub>1ā€“<i>x</i></sub>Mo<sub><i>x</i></sub>O<sub>4</sub> (<i>x</i> ā‰¤ 0.3) compounds are spin-frustrated materials that have higher magnetic and ferroelectric phase-transition temperatures than does pure MnWO<sub>4</sub>
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