2 research outputs found

    Downscaling Effect on the Superconductivity of Pd<sub>3</sub>Bi<sub>2</sub>X<sub>2</sub> (X = S or Se) Nanoparticles Prepared by Microwave-Assisted Polyol Synthesis

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    Pd<sub>3</sub>Bi<sub>2</sub>S<sub>2</sub> and Pd<sub>3</sub>Bi<sub>2</sub>Se<sub>2</sub> have been successfully prepared in the form of nanoparticles with diameters of ∼50 nm by microwave-assisted modified polyol synthesis at low temperatures. The composition and morphology of the samples have been studied by means of powder X-ray diffraction as well as electron microscopy methods, including X-ray intensity mapping on the nanoscale. Superconducting properties of the as-prepared samples have been characterized by electrical resistivity measurements down to low temperatures (∼0.2 K). Deviations from the bulk metallic behavior originating from the submicrometer nature of the samples were registered for both phases. A significant critical-field enhancement up to 1.4 T, i.e., 4 times higher than the value of the bulk material, has been revealed for Pd<sub>3</sub>Bi<sub>2</sub>Se<sub>2</sub>. At the same time, the critical temperature is suppressed to 0.7 K from the bulk value of ∼1 K. A superconducting transition at 0.4 K has been observed in nanocrystalline Pd<sub>3</sub>Bi<sub>2</sub>S<sub>2</sub>. Here, a zero-temperature upper critical field of ∼0.5 T has been estimated. Further, spark plasma-sintered Pd<sub>3</sub>Bi<sub>2</sub>S<sub>2</sub> and Pd<sub>3</sub>Bi<sub>2</sub>Se<sub>2</sub> samples have been investigated. Their superconducting properties are found to lie between those of the bulk and nanosized samples

    Synthesis of a Cu-Filled Rh<sub>17</sub>S<sub>15</sub> Framework: Microwave Polyol Process Versus High-Temperature Route

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    Metal-rich, mixed copper–rhodium sulfide Cu<sub>3−δ</sub>Rh<sub>34</sub>S<sub>30</sub> that represents a new Cu-filled variant of the Rh<sub>17</sub>S<sub>15</sub> structure has been synthesized and structurally characterized. Copper content in the [CuRh<sub>8</sub>] cubic cluster was found to vary notably dependent on the chosen synthetic route. Full site occupancy was achieved only in nanoscaled Cu<sub>3</sub>Rh<sub>34</sub>S<sub>30</sub> obtained by a rapid, microwave-assisted reaction of CuCl, Rh<sub>2</sub>(CH<sub>3</sub>CO<sub>2</sub>)<sub>4</sub> and thiosemicarbazide at 300 °C in just 30 min; whereas merely Cu-deficient Cu<sub>3−δ</sub>Rh<sub>34</sub>S<sub>30</sub> (2.0 ≥ δ ≥ 0.9) compositions were realized via conventional high-temperature ceramic synthesis from the elements at 950 °C. Although Cu<sub>3−δ</sub>Rh<sub>34</sub>S<sub>30</sub> is metallic just like Rh<sub>17</sub>S<sub>15</sub>, the slightly enhanced metal content has a dramatic effect on the electronic properties. Whereas the Rh<sub>17</sub>S<sub>15</sub> host undergoes a superconducting transition at 5.4 K, no signs of the latter were found for the Cu-derivatives at least down to 1.8 K. This finding is corroborated by the strongly reduced density of states at the Fermi level of the ternary sulfide and the disruption of long-range Rh–Rh interactions in favor of Cu–Rh interactions as revealed by quantum-chemical calculations
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