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Non-Cuprate-Planar Superconductivity
Authors:John D Dow and Dale R Harshman
Affiliation:(1) Department of Physics, Arizona State University, Tempe, Arizona, 85287;(2) Physikon Research Corporation, P.O. Box 1014, Lynden, Washington, 98264
Abstract:The ruthenate compounds, Gd2–zCe z Sr2Cu2RuO10, GdSr2Cu2RuO8, and doped Sr2YRuO6, all superconduct in their SrO layers, which is why they have almost the same sim49 K onset temperatures for superconductivity. The sister compound Ba2GdRuO6, either doped or not, does not superconduct, because L = 0, J ne 0 Gd breaks pairs and destroys superconductivity in the potentially superconducting BaO layers. High-temperature superconductivity resides in the SrO or BaO layers, or in interstitial-oxygen regions of the crystal, not in the cuprate-planes.
Keywords:theories and models of the superconducting state  type II superconductivity  high-Tc compounds
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