A unified explanation of the Kadowaki–Woods ratio in strongly correlated metals

Abstract

The Kadowaki–Woods ratio attempts to relate the temperature dependence of a metal to its heat capacity. However, as it takes different values for different classes of metals it is not universal. By including effects related to carrier density and spatial dimensionality, a much more universal ratio, which describes the properties of many different systems, has been achieved. Discoveries of ratios whose values are constant within broad classes of materials have led to many deep physical insights. The Kadowaki–Woods ratio (KWR; refs 1, 2) compares the temperature dependence of a metal’s resistivity to that of its heat capacity, thereby probing the relationship between the electron–electron scattering rate and the renormalization of the electron mass. However, the KWR takes very different values in different materials3,4. Here we introduce a ratio, closely related to the KWR, that includes the effects of carrier density and spatial dimensionality and takes the same (predicted) value in organic charge-transfer salts, transition-metal oxides, heavy fermions and transition metals—despite the numerator and denominator varying by ten orders of magnitude. Hence, in these materials, the same emergent physics is responsible for the mass enhancement and the quadratic temperature dependence of the resistivity, and no exotic explanations of their KWRs are required.

Cite this article

Jacko, A., Fjærestad, J. & Powell, B. A unified explanation of the Kadowaki–Woods ratio in strongly correlated metals. Nature Phys 5, 422–425 (2009). https://doi.org/10.1038/nphys1249

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