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   <subfield code="a">Magnetic and Superconducting Properties of Doped and Undoped Double Perovskite Sr2YRuO6</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[S. Rao, J. Srivastava, M. Wu, B. Mok, C. Chen, M. Ling, H.-L. Liu, Y. Chen, J. Ho]</subfield>
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   <subfield code="a">We report here SQUID (magnetization) measurements, along with supporting specific heat, Raman, SEM (scanning electron microscope), EDX (energy dispersive X-ray) and XRD (X-ray diffraction) measurements, on Cu-doped and undoped double perovskite $\mathrm{Sr}_{2}^{2+}\mathrm{Y}^{3+}\mathrm{Ru}^{5+}\mathrm{O}_{6}^{2-}$ (abbreviated as SrY2116) system grown as single crystal using high-temperature solution growth technique. These measurements show the undoped system to be a nonmetallic (insulating) spin glass (SG) and the ∼5-30% Cu-doped (i.e. Cu-concentration/(Cu + Ru-concentration) ∼5-30%) system to be a spin glass superconductor (SGSC) with T c (critical temperature) ∼28-31K and superconducting volume fraction, f sc∼2.2-9%. To mention, similar measurements done on undoped and Cu-doped BaY2116 and BaPr2116 systems show for them the same (SG, SGSC) behaviors. However they show a decrease in T c and f sc when diamagnetic Y3+ ions are replaced by Pr3+ spins, presumably due to enhanced internal pair breaking, and also decreased Cu-O-Cu overlap, owing to Pr3+ presence; these phenomena are known to exist in the Pr123 compound, PrBa2Cu3O7−δ (δ∼0), due to ∼10% of Pr3+ ions having tendency to occupy Ba2+ sites. Measurements done on undoped and Cu-doped SrHo2116 show similar SG and SGSC properties. Further, the undoped and Cu-doped SrY2116 crystals grown by hydrothermal growth technique (i.e., grown using lower temperature and high pressure) show same behaviors. From these investigations it can be said that the undoped Ru-double perovskites (A2BB′O6, B′=Ru) are SG systems and that Cu-doped Ru-double perovskites (A2BB′Oδ, δ∼6, B′=Ru1−x Cux, 0&lt;x≲0.3) are SG superconductors (SGSCs). Results are discussed.</subfield>
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   <subfield code="a">Springer Science+Business Media, LLC, 2010</subfield>
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   <subfield code="a">Double perovskite</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">Ruthenocuprate</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">High- T c superconductivity</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">Magnetic superconductor</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">Frustration</subfield>
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   <subfield code="a">Spin glass</subfield>
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   <subfield code="a">Rao</subfield>
   <subfield code="D">S.</subfield>
   <subfield code="u">Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan (ROC)</subfield>
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   <subfield code="a">Srivastava</subfield>
   <subfield code="D">J.</subfield>
   <subfield code="u">Tata Institute of Fundamental Research, 400005, Mumbai, India</subfield>
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   <subfield code="a">Wu</subfield>
   <subfield code="D">M.</subfield>
   <subfield code="u">Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan (ROC)</subfield>
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   <subfield code="a">Mok</subfield>
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   <subfield code="u">Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan (ROC)</subfield>
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   <subfield code="a">Chen</subfield>
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   <subfield code="u">Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan (ROC)</subfield>
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   <subfield code="D">M.</subfield>
   <subfield code="u">Department of Physics, National Taiwan Normal University, 116, Taipei, Taiwan (ROC)</subfield>
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   <subfield code="u">Department of Physics, Wichita State University, 67260-0032, Wichita, KS, USA</subfield>
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   <subfield code="t">Journal of Superconductivity and Novel Magnetism</subfield>
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   <subfield code="g">24/4(2011-05-01), 1249-1262</subfield>
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