Conductivity and anomalous Hall effect in film magnetic nanocomposites based on nonstoichiometric oxides
- Authors: 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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Affiliations:
- National Research Center “Kurchatov Institute,”
- Moscow State University
- Voronezh State Technical University
- Institute of Theoretical and Applied Electrodynamics
- Issue: Vol 11, No 3 (2017)
- Pages: 549-553
- Section: Article
- URL: https://journal-vniispk.ru/1027-4510/article/view/193027
- DOI: https://doi.org/10.1134/S1027451017030132
- ID: 193027
Cite item
Abstract
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.
About the authors
S. N. Nikolaev
National Research Center “Kurchatov Institute,”
Author for correspondence.
Email: niklser@list.ru
Russian Federation, Moscow, 123182
K. Yu. Chernoglazov
National Research Center “Kurchatov Institute,”
Email: niklser@list.ru
Russian Federation, Moscow, 123182
V. A. Demin
National Research Center “Kurchatov Institute,”
Email: niklser@list.ru
Russian Federation, Moscow, 123182
N. K. Chumakov
National Research Center “Kurchatov Institute,”
Email: niklser@list.ru
Russian Federation, Moscow, 123182
V. A. Levanov
National Research Center “Kurchatov Institute,”; Moscow State University
Email: niklser@list.ru
Russian Federation, Moscow, 123182; Moscow, 119991
A. A. Magomedova
Moscow State University
Email: niklser@list.ru
Russian Federation, Moscow, 119991
A. V. Sitnikov
Voronezh State Technical University
Email: niklser@list.ru
Russian Federation, Voronezh, 394026
Yu. E. Kalinin
Voronezh State Technical University
Email: niklser@list.ru
Russian Federation, Voronezh, 394026
A. B. Granovskii
Moscow State University; Institute of Theoretical and Applied Electrodynamics
Email: niklser@list.ru
Russian Federation, Moscow, 119991; Moscow, 127412
V. V. Rilkov
National Research Center “Kurchatov Institute,”; Institute of Theoretical and Applied Electrodynamics
Email: niklser@list.ru
Russian Federation, Moscow, 123182; Moscow, 127412
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