16 research outputs found
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Structural and magnetic investigation of Fe3+ and Mg2+ substitution into the trigonal bipyramidal site of InGaCuO4
The solid solutions of InGa₁₋ₓFeₓCuO₄, InFeCu₁₋ₓMgₓO₄, and InGa₁₋ₓFeₓCu₁₋ₓMgₓO₄ were
synthesized and characterized through the use of X – ray and neutron diffraction, and DC –
magnetism measurements. All compositions of InGa₁₋ₓFeₓCuO₄ are single phase and crystallize
in the R3m space group, but a transformation to the spinel InFeMgO₄ structure was observed for
the other series of Fe³⁺ and Mg²⁺ − rich compounds. As a result of the similar ionic radii for
Ga³⁺ and Fe³⁺, there was not an obvious change in the c/a ratio for InGa₁₋ₓFeₓCuO₄. In the
hexagonal domains, the c/a ratio of InFeCu₁₋ₓMgₓO₄ and InGa₁₋ₓFeₓCu₁₋ₓMgₓO₄ showed a linear
trend that can be explained by the change in electronic configurations between Cu²⁺ and Mg²⁺.
All hexagonal compositions display negative Weiss temperatures, and there is an increase in the
magnetic transition temperature with the addition of Fe³⁺. Additional AC magnetic susceptibility
measurements for the x = 0.4 and 0.6 compositions within the InGa₁₋ₓFeₓCuO₄ solid solution
show that these transitions are consistent with spin glass behavior, not long range AFM ordering
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Structural and magnetic investigation of In₂Fe₂₋ₓGaₓCuO₇
The solid solution of In₂Fe₂₋ₓGaₓCuO₇ (space group P6₃/mmc) was synthesized and investigated through X-ray diffraction and magnetic susceptibility studies. Limited changes to the lattice parameters were observed as a result of the similar ionic radii for Fe³⁺ and Ga³⁺ in the trigonal bipyramidal (TBP) crystallographic site. An increase in the Weiss temperature, along with spin glass behavior are observed from x = 0 – 2, but irregularities in the trend are apparent for x = 0.75 and 1. With the highest concentration in magnetic ions, In₂Fe₂CuO₇ appears to have competing nearest neighbor interactions that produce a suppression of the Curie tail and the experimental magnetic moment. In comparison to InFe₁₋ₓGaₓCuO₄, both solid solutions show an invariable progression of the lattice parameters, but the magnetic properties are greatly affected by the distinct TBP layering schemes.Keywords: X – ray diffraction, Layered compounds, Trigonal bipyramidal coordination, Transition metal oxides, Magnetic propertiesKeywords: X – ray diffraction, Layered compounds, Trigonal bipyramidal coordination, Transition metal oxides, Magnetic propertie
Influence of Structural Disorder on Hollandites A<sub><i>x</i></sub>Ru<sub>4</sub>O<sub>8</sub> (A<sup>+</sup> = K, Rb, Rb<sub>1–<i>x</i></sub>Na<sub><i>x</i></sub>)
Influence of Structural Disorder on Hollandites A<sub><i>x</i></sub>Ru<sub>4</sub>O<sub>8</sub> (A<sup>+</sup> = K, Rb, Rb<sub>1–<i>x</i></sub>Na<sub><i>x</i></sub>)
Structural
disorder can play an important role in the electrical properties of
correlated materials. In this work we examine the average and local
disorder in hollandites A<sub><i>x</i></sub>Ru<sub>4</sub>O<sub>8</sub> (A<sup>+</sup> = K, Rb, Rb<sub>1–<i>x</i></sub>Na<sub><i>x</i></sub>) through neutron total scattering
techniques. Samples with A<sup>+</sup> = Rb, Rb<sub>1–<i>x</i></sub>Na<sub><i>x</i></sub> exhibit the largest
amount of local disorder as evidenced by higher atomic displacement
parameters, and as a result, a weakened temperature dependence of
the resistivity is observed upon cooling as compared to K<sub><i>x</i></sub>Ru<sub>4</sub>O<sub>8</sub>. All samples exhibit
anisotropic resistivity that is dominated by metallic conductivity
at lower temperatures, and this is corroborated by Pauli paramagnetic
behavior throughout the measured temperature regime
