Ferromagnetic behavior of the Ru sub(1-) sub(x)Sr sub(2GdCu) sub(2)+ sub(xO) sub(8)+/- sub(z system with 0.0~~ZZ: x~~ZZ: 1.0, synthesized at ambient pressure)
The Ru sub(1-) sub(x)Sr sub(2GdCu) sub(2)+ sub(xO) sub(8)+/- sub(z system with x = 0.0, 0.1, 0.2, 0.3, 0.4, 0.9 and 1.0 was studied by differential thermal analysis (DTA) in air in order to determine the temperature interval at which the formation of the RuSr) sub(2)GdCu sub(2O) sub(8) (Ru-1212) com...
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Published in | Physica. C, Superconductivity Vol. 468; no. 21; pp. 2219 - 2223 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
Published |
01.10.2008
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Subjects | |
Online Access | Get full text |
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Summary: | The Ru sub(1-) sub(x)Sr sub(2GdCu) sub(2)+ sub(xO) sub(8)+/- sub(z system with x = 0.0, 0.1, 0.2, 0.3, 0.4, 0.9 and 1.0 was studied by differential thermal analysis (DTA) in air in order to determine the temperature interval at which the formation of the RuSr) sub(2)GdCu sub(2O) sub(8) (Ru-1212) compound should be formed. For DTA data, samples were prepared by the solid-state reaction method at ambient pressure between 940 degree C and 1050 degree C. From the X-ray powder diffraction (XRD) patterns it was observed that this system is isostructural to the Ru-1212 compound. In addition, a pure phase up to x = 0.4 was obtained. Studies by the Scanning Electron Microscopy (SEM) technique produced a particle size around 1-5 mu m. The results of Transmission Electronic Microscopy (TEM) studies confirm the tetragonal unit cell in the Ru sub(1-) sub(x)Sr sub(2GdCu) sub(2)+ sub(xO) sub(8)+/- sub(z system. The temperature dependence of the electrical resistivity of the samples with x = 0.1, 0.2 and 0.4 annealed in oxygen flux for 6, 12 and 41 h, at T = 960 degree C, shows a semiconducting behavior. The AC magnetic susceptibility measurement indicates ferromagnetic behavior with T) super(C)urie between 130 and 138 K. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 content type line 23 ObjectType-Feature-1 |
ISSN: | 0921-4534 |
DOI: | 10.1016/j.physc.2008.06.006 |