Theory of the anomalous Hall effect in heavy-fermion systems

H. Kohno; K. Yamada; S. Inagaki

doi:10.1016/0921-4526(93)90740-W

Theory of the anomalous Hall effect in heavy-fermion systems

H. Kohno, K. Yamada, S. Inagaki

Department of Physics

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Abstract

The Fermi-liquid theory is further developed for the anomalous Hall effect due to skew scattering on the basis of the periodic Anderson model with degenerate orbitals and spin-orbit coupling. In the low-temperature coherent regime, the skew-scattering contribution to the Hall coefficient is generally proportional to the square of the total resistivity. At low temperatures, this relation is in good agreement with experiments on several Ce and U compounds.

Original language	English
Pages (from-to)	910-912
Number of pages	3
Journal	Physica B: Physics of Condensed Matter
Volume	186-188
Issue number	C
DOIs	https://doi.org/10.1016/0921-4526(93)90740-W
Publication status	Published - 1993 May 2

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Condensed Matter Physics
Electrical and Electronic Engineering

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10.1016/0921-4526(93)90740-W

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title = "Theory of the anomalous Hall effect in heavy-fermion systems",

abstract = "The Fermi-liquid theory is further developed for the anomalous Hall effect due to skew scattering on the basis of the periodic Anderson model with degenerate orbitals and spin-orbit coupling. In the low-temperature coherent regime, the skew-scattering contribution to the Hall coefficient is generally proportional to the square of the total resistivity. At low temperatures, this relation is in good agreement with experiments on several Ce and U compounds.",

author = "H. Kohno and K. Yamada and S. Inagaki",

year = "1993",

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AU - Inagaki, S.

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AB - The Fermi-liquid theory is further developed for the anomalous Hall effect due to skew scattering on the basis of the periodic Anderson model with degenerate orbitals and spin-orbit coupling. In the low-temperature coherent regime, the skew-scattering contribution to the Hall coefficient is generally proportional to the square of the total resistivity. At low temperatures, this relation is in good agreement with experiments on several Ce and U compounds.

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Theory of the anomalous Hall effect in heavy-fermion systems

Abstract

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