Abstract
A mean-field description is given for spin glass systems without ideal classical local moments. The starting point is a moderately dilute set of Anderson model impurities, each with a finite Kondo or spin fluctuation temperature, coupled by indirect exchange. The results are consistent with a picture in which the Kondo and spin glass interactions compete, leading to the existence of a finite concentration threshold for T = 0 spin glass behavior.
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Hertz, J.A. (1981). Stoner and Kondo Spin Glasses. In: Moriya, T. (eds) Electron Correlation and Magnetism in Narrow-Band Systems. Springer Series in Solid-State Sciences, vol 29. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-81639-0_16
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DOI: https://doi.org/10.1007/978-3-642-81639-0_16
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