Conductivity and anomalous Hall effect in film magnetic nanocomposites based on nonstoichiometric oxides
- Autores: Nikolaev S.N.1, Chernoglazov K.Y.1, Demin V.A.1, Chumakov N.K.1, Levanov V.A.1,2, Magomedova A.A.2, Sitnikov A.V.3, Kalinin Y.E.3, Granovskii A.B.2,4, Rilkov V.V.1,4
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Afiliações:
- National Research Center “Kurchatov Institute,”
- Moscow State University
- Voronezh State Technical University
- Institute of Theoretical and Applied Electrodynamics
- Edição: Volume 11, Nº 3 (2017)
- Páginas: 549-553
- Seção: Article
- URL: https://journals.rcsi.science/1027-4510/article/view/193027
- DOI: https://doi.org/10.1134/S1027451017030132
- ID: 193027
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Resumo
The transport properties of film nanocomposites (Co40Fe40B20)x(AlOy)100 − x and (Co84Nb14Ta2)x(AlOy)100 − x based on AlOy oxide (y ~ 1), containing a ferromagnetic metal, are studied in the region of the metal–insulator transition (57 > x > 47 at %). It is found that at x > 49 at %, the conductivity of nanocomposites is well described by a logarithmic law of σ(T) = a + b ln T, which can be explained by the peculiarities of the Coulomb interaction in nanogranular systems with metallic conductivity near the metal—insulator transition. It is shown that parameter b is determined by the characteristic size of the percolation cluster cell, which in nanocomposites of both types happen to be the same (~8 nm) and correlates well with the results of electron microscopy studies. The temperature dependence of the anomalous Hall effect at the logarithmic dependence of conductivity is studied for the first time. In the immediate vicinity of the transition, a power-law scaling between the anomalous Hall resistance and longitudinal resistance ρHa ∝ ρ0.4, is detected, which can be explained by the suppression of its own mechanism of the anomalous Hall effect under the strong scattering of charge carriers.
Sobre autores
S. Nikolaev
National Research Center “Kurchatov Institute,”
Autor responsável pela correspondência
Email: niklser@list.ru
Rússia, Moscow, 123182
K. Chernoglazov
National Research Center “Kurchatov Institute,”
Email: niklser@list.ru
Rússia, Moscow, 123182
V. Demin
National Research Center “Kurchatov Institute,”
Email: niklser@list.ru
Rússia, Moscow, 123182
N. Chumakov
National Research Center “Kurchatov Institute,”
Email: niklser@list.ru
Rússia, Moscow, 123182
V. Levanov
National Research Center “Kurchatov Institute,”; Moscow State University
Email: niklser@list.ru
Rússia, Moscow, 123182; Moscow, 119991
A. Magomedova
Moscow State University
Email: niklser@list.ru
Rússia, Moscow, 119991
A. Sitnikov
Voronezh State Technical University
Email: niklser@list.ru
Rússia, Voronezh, 394026
Yu. Kalinin
Voronezh State Technical University
Email: niklser@list.ru
Rússia, Voronezh, 394026
A. Granovskii
Moscow State University; Institute of Theoretical and Applied Electrodynamics
Email: niklser@list.ru
Rússia, Moscow, 119991; Moscow, 127412
V. Rilkov
National Research Center “Kurchatov Institute,”; Institute of Theoretical and Applied Electrodynamics
Email: niklser@list.ru
Rússia, Moscow, 123182; Moscow, 127412
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