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      Synthesis and physical properties of perovskite Sm 1−x Sr x NiO 3 (x = 0, 0.2) and infinite-layer Sm 0.8Sr 0.2NiO 2 nickelates

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      Journal of Physics: Condensed Matter
      IOP Publishing

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          Abstract

          Recently, superconductivity at about 9–15 K was discovered in Nd 1− x Sr x NiO 2 (Nd-112, x ≈ 0.125–0.25) infinite-layer thin films, which has stimulated enormous interests in related rare-earth nickelates. Usually, the first step to synthesize this 112 phase is to fabricate the RNiO 3 ( R-113, R: rare-earth element) phase, however, it was reported that the 113 phase is very difficult to be synthesized successfully due to the formation of unusual Ni 3+ oxidation state. And the difficulty of preparation is enhanced as the ionic radius of rare-earth element decreases. In this work, we report the synthesis and investigation on multiple physical properties of polycrystalline perovskites Sm 1− x Sr x NiO 3 ( x = 0, 0.2) in which the ionic radius of Sm 3+ is smaller than that of Pr 3+ and Nd 3+ in related superconducting thin films. The structural and compositional analyses conducted by x-ray diffraction and energy dispersive x-ray spectrum reveal that the samples mainly contain the perovskite phase of Sm 1− x Sr x NiO 3 with small amount of NiO impurities. Magnetization and resistivity measurements indicate that the parent phase SmNiO 3 undergoes a paramagnetic–antiferromagnetic transition at about 224 K on a global insulating background. In contrast, the Sr-doped sample Sm 0.8Sr 0.2NiO 3 shows a metallic behavior from 300 K down to about 12 K, while below 12 K the resistivity exhibits a slight logarithmic increase. Meanwhile, from the magnetization curves, we can see that a possible spin-glass state occurs below 12 K in Sm 0.8Sr 0.2NiO 3. Using a soft chemical reduction method, we also obtain the infinite-layer phase Sm 0.8Sr 0.2NiO 2 with square NiO 2 planes. The compound shows an insulating behavior which can be described by the three-dimensional variable-range-hopping model. And superconductivity is still absent in the polycrystalline Sm 0.8Sr 0.2NiO 2.

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          • Record: found
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          From quantum matter to high-temperature superconductivity in copper oxides.

          The discovery of high-temperature superconductivity in the copper oxides in 1986 triggered a huge amount of innovative scientific inquiry. In the almost three decades since, much has been learned about the novel forms of quantum matter that are exhibited in these strongly correlated electron systems. A qualitative understanding of the nature of the superconducting state itself has been achieved. However, unresolved issues include the astonishing complexity of the phase diagram, the unprecedented prominence of various forms of collective fluctuations, and the simplicity and insensitivity to material details of the 'normal' state at elevated temperatures.
            Bookmark
            • Record: found
            • Abstract: not found
            • Article: not found

            A profile refinement method for nuclear and magnetic structures

              Bookmark
              • Record: found
              • Abstract: not found
              • Article: not found

              Possible highT c superconductivity in the Ba?La?Cu?O system

                Bookmark

                Author and article information

                Contributors
                Journal
                Journal of Physics: Condensed Matter
                J. Phys.: Condens. Matter
                IOP Publishing
                0953-8984
                1361-648X
                May 25 2021
                June 30 2021
                May 25 2021
                June 30 2021
                : 33
                : 26
                : 265701
                Article
                10.1088/1361-648X/abfb90
                c92757d2-4eac-422c-abaf-e2f8d3349dae
                © 2021

                https://iopscience.iop.org/page/copyright

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