Abstract
In previous chapters, we have explained the significant role of the CVC in the presence of AF fluctuations. For example, \(R_{\mathrm{{H}}}\) shows strong temperature dependence due to the CVC. This mechanism of non-Fermi-liquid-like behaviors occurs not only in single-band systems like cuprates, but also in multiband systems like \(\mathrm{{CeMIn}}_5\) (\(M=Co, Rh, Ir\)).
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Notes
- 1.
In Refs. [4, 5], we put \(=(\pi T)^2/6\cdot N_{\!f}\rho ^f(0)\) by mistake; the correct relation is \(\gamma =(\pi T)^2/3\cdot N_{\!f}\rho ^f(0)\). For this reason, Eq. (10.13) is two times Eq. (8) in Ref. [4]. Since the author of Ref. [4] assumed \(1/n^{4/3}a^{3} \approx 1\times 10^{-8}\) cm, the grand-KW relation in Ref. [4] is equal to Eq. (10.15) in the present paper.
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Kontani, H. (2013). Multiorbital Systems. In: Transport Phenomena in Strongly Correlated Fermi Liquids. Springer Tracts in Modern Physics, vol 251. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-35365-9_10
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