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Titlebook: Electronic Conduction in Oxides; Nobuo Tsuda,Keiichiro Nasu,Kiiti Siratori Textbook 19911st edition Springer-Verlag Berlin Heidelberg 1991

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0171-1873 in 1983 as the second volume of the Material Science Series, which was edited for postgraduate students by T. Suzuki, S. Chikazumi, and S. Nakajima. Since the publication of the first edition, we have witnessed the historic discovery of high-Tc superconductors by J. G. Bednorz and K. A. Müller. Tbe
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Introduction,and brittle. They remain brittle even at room temperature, except for a certain specially fabricated zirconium oxide. However as far as their electrical properties are concerned, there are actually many good conductors and in fact thallium-copper oxide shows superconductivity at temperatures as high as 125 K.
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Prevention of White Spot Lesions,termost orbitals of the atoms or molecules constituting each crystal. Consequently, one of the most important problems in the solid state theory is to find the relation between the microscopic nature of the outermost electrons and the macroscopic properties of solids.
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Textbook 19911st edition present status of theoretical studies of the electron-phonon interaction in solids and Yanase explains the electron correlation. Chapter 4 treats the physics ofvarious representative oxides in detail. Sections 4. 1-5 and 4. 10 were written by Tsuda and Sects. 4. 6-9 by Siratori. This chapter is int
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Introduction, as aluminium, copper, and iron. Metals can carry an electric current and are ductile, whereas oxides have generally been considered to be insulating and brittle. They remain brittle even at room temperature, except for a certain specially fabricated zirconium oxide. However as far as their electric
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Theories for Many-Body Problems in Strongly Coupled Electron-Phonon Systems, and optical properties, which change from one crystal to the other. The difference of these macroscopic properties between crystals mainly originates from the difference of the microscopic nature of electrons in each crystal. Especially, it mainly comes from the outer electrons, which are in the ou
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