Titlebook: Electron Correlations and Materials Properties; A. Gonis,N. Kioussis,M. Ciftan Book 1999 Springer Science+Business Media New York 1999 Met

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明確

Edda Weimann MD, MPH,Peter Weimann MSci, PhDrstand the basic phenomena responsible for these properties. The reader is referred to numerous review articles, such as Fisk et al., (1995), Grewe and Steglich (1991), Hess et al., (1993), Lawrence and Mills (1991), Ott and Fisk (1987), Stewart (1984), Thompson and Lawrence (1994). The term heavy f

Narcissist

unstable-angina

Integration of INS and GPS Measurementsk of Johansson and his collaborators (Johansson et al., 1981) we know that these effects arise from interactions involving the 5f electrons. Progress in theory is bringing these effects within the range of detailed theoretical calculation: we have prepared this article to summarize the experimental

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André J. R. Péqueux,Raymond Gillesf actinide neighbors and wave functions of valence electrons of other ligands in alloys and intermetallic compounds. Consequently, the original actinide free-ion character of . electron states is modified to smaller or larger extent depending on the geometry of the actinide ion neighborhood and the

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CORE

Hydrostatic Pressure Apparatus,erconducting phase transition below 2 K without destruction of the ordered magnetic moment. In the superconducting phase the low energy magnetic inelastic response is qualitatively of a different form from that above T.,. We review this low energy response.

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Surinder M. Sharma,Rajagopala Chidambaram f shells is embedded in a metallic environment. Below a characteristic “Kondo temperature” T., typically of the order of 10K, quasiparticles composed of both local f degrees of freedom and itinerant conduction-electron degrees of freedom form. As has been inferred from the giant Sommerfeld coeffici