Abstract
A theory of the generalized conductivity for the normal component of the Hall effect is developed. It is shown that the normal Hall effect coefficient R 0 of microscopically inhomogeneous magnetic alloys GdZnxCu1−x , which at low temperatures consist of ferro-, antiferro-, and paramagnetic phases, can be described satisfactorily on the basis of an effective-medium theory. The experimentally observed relationship between the coefficient R 0(x) and the resistivity ρ(x) is obtained.
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Fiz. Tverd. Tela (St. Petersburg) 41, 98–102 (January 1999)
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Mityushov, E.A., Kourov, N.I. & Irkhin, Y.P. Hall effect in microscopically inhomogeneous magnetic alloys. Phys. Solid State 41, 87–90 (1999). https://doi.org/10.1134/1.1130734
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DOI: https://doi.org/10.1134/1.1130734