Analysis of the magnetoresistance contributions in a nanocrystallized Cr-doped FINEMET alloy |
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Authors: | L.F. KissV. Franco,M. CsontosL. Pé ter,C.F. CondeA. Conde,T. Kemé nyJ. Tó th,L.K. VargaI. Bakonyi |
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Affiliation: | a Research Institute for Solid State Physics and Optics, Hungarian Academy of Sciences, H-1525 Budapest, P.O. Box 49, Hungary b Departamento de Física de la Materia Condensada, Instituto de Ciencia de Materiales C.S.I.C., Universidad de Sevilla, Apartado 1065, 41080 Sevilla, Spain c Department of Physics, Institute of Physics, Budapest University of Technology and Economics and Research Group of the Hungarian Academy of Sciences, H-1111 Budapest, Budafoki út 6-8, Hungary |
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Abstract: | The magnetoresistance (MR) was measured at 200, 250 and 300 K in magnetic fields up to B=12 T for a nanocrystallized Fe63.5Cr10Nb3Cu1Si13.5B9 alloy. Both the longitudinal (LMR) and transverse (TMR) component of the magnetoresistance decreased from B=0 to about 0.1 T. This could be ascribed to a giant MR (GMR) effect due to spin-dependent scattering of conduction electrons along their path between two Fe-Si nanograins via the non-magnetic matrix. Such a scattering may occur if the nanograin moments are not or only weakly coupled in the absence of a strong exchange coupling (due to the high Cr content in the matrix) and/or only weak dipole-dipole coupling is present (due to sufficiently large separations between the nanograins). For larger fields, the GMR saturated and a slightly nonlinear increase in MR with B was observed due to a contribution by the residual amorphous matrix. The anisotropic MR effect (AMR≡LMR−TMR) was negative for all fields and temperatures investigated. By measuring the MR of melt-quenched Fe100−xSix solid solutions with x=15, 18, 20, 25 and 28, the observed AMR could be identified as originating from the Fe-Si nanograins having a D03 structure. |
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Keywords: | Magnetoresistance Amorphous alloys Nanocrystallization FINEMET alloys Fe-Si alloys |
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