Abstract
The unusual properties of heavy fermion (or heavy electron) materials have sparked an avalanche of research over the last two decades in order to understand 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 fermion refers to materials (thus far only compounds with elements having an unfilled 4f or 5f shells) whose electronic properties suggest that the conduction electrons have a very heavy effective mass. This is inferred from the linear term in the low specific heat (Cp = γT+ OT2) which usually has an upturn at low temperatures and suggests [some of the first discoveries were by Andres et al. (1975), followed by Steglich (1979), Stewart et al (1984), Ott et al. (1983)1 y-values as large as 1500 mJ/mole-K2. deHaas-van Alphen measurements have confirmed the existence of heavy masses [Springford and Reinders (1988), Lonzarich (1988), Onuki (1993)1. The quadratic term in the resistivity and the Pauli susceptibility also indicate the existence of a mass enhancement. It is well established that indeed it is the f-electrons that are responsible for the unusual properties [Grewe and Steglich (1991)].
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Arko, A.J. et al. (1999). Photoemission in Strongly Correlated Crystalline f-Electron Systems: A Need for a New Approach. In: Gonis, A., Kioussis, N., Ciftan, M. (eds) Electron Correlations and Materials Properties. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-4715-0_3
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