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Anomalous Hall effect in (Co41Fe39B20) x (Al-O)100 − x nanocomposites

Yu. O. MikhailovskyFaculty of Physics, Moscow State University, Moscow, 119991, RussiaDenis MettusFaculty of Physics, Moscow State University, Moscow, 119991, RussiaAlexander KazakovFaculty of Physics, Moscow State University, Moscow, 119991, RussiaV. N. PrudnikovMoscow State UniversityYu. E. KalininVoronezh State Technical University, Voronezh, 394026, RussiaA. S. SitnikovVoronezh State Technical University, Voronezh, 394026, RussiaA. GerberRaymond and Beverly Sackler Faculty of Exact Sciences, School of Physics and Astronomy, Tel Aviv University, Ramat Aviv, Tel Aviv, 69978, IsraelD. BartovRaymond and Beverly Sackler Faculty of Exact Sciences, School of Physics and Astronomy, Tel Aviv University, Ramat Aviv, Tel Aviv, 69978, IsraelA. B. GranovskyFaculty of Physics, Moscow State University, Moscow, 119991, Russia
2013en
ABI

Abstract

The concentration dependence of the coefficient R s characterizing the anomalous Hall effect (AHE) has been studied by measuring the electrical resistivity ρ, magnetoresistance, and the magnetic field dependence of magnetization and Hall resistivity of (Co41Fe39B20) x (Al-O)100 − x nanocomposite thin films. It has been demonstrated that the AHE coefficient increases by more than an order of magnitude with a decrease in the percentage x of the amorphous ferromagnetic metal from 60 to 30 and its behavior is described by the relation R s ∼ ρ m , where m = 0.46 ± 0.1. At the same time, the coefficient characterizing the normal Hall effect grows by a factor of less than 10. The mechanisms underlying the giant Hall effect in nanocomposites have been discussed.

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