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Magnetization dynamics in an exchange-coupled NiFe/CoFe bilayer studied by x-ray detected ferromagnetic resonance

DOI: 10.1088/1367-2630/17/1/013019 DOI Help

Authors: G. Stenning (University of Southampton; ISIS) , L. Shelford (Diamond Light Source) , S. Cavill (University of York, Diamond Light Source) , F. Hoffmann (Universität Regensburg) , M. Haertinger (Universität Regensburg) , T. Hesjedal (University of Oxford) , G. Woltersdorf (Martin-Luther-Universität Halle-Wittenberg) , G. Bowden (University of Southampton) , S A Gregory (University of Southampton) , C. Back (Fakultät für Physik, Universität Regensburg, Universitätsstrasse 31, 93040 Regensburg) , P. De Groot (University of Southampton) , G. Van Der Laan (Diamond Light Source)
Co-authored by industrial partner: No

Type: Journal Paper
Journal: New Journal Of Physics , VOL 17

State: Published (Approved)
Published: January 2015
Diamond Proposal Number(s): 7745

Open Access Open Access

Abstract: Exchange-coupled hard and soft magnetic layers find extensive use in data storage applications, for which their dynamical response has great importance. With bulk techniques, such as ferromagnetic resonance (FMR), it is difficult to access the behaviour and precise influence of each individual layer. By contrast, the synchrotron radiation-based technique of x-ray detected ferromagnetic resonance (XFMR) allows element-specific and phase-resolved FMR measurements in the frequency range 0.5–11 GHz. Here, we report the study of the magnetization dynamics of an exchange-coupled Ni0.81Fe0.19 (43.5 nm)/Co0.5Fe0.5 (30 nm) bilayer system using magnetometry and vector network analyser FMR, combined with XFMR at the Ni and Co L2 x-ray absorption edges. The epitaxially grown bilayer exhibits two principal resonances denoted as the acoustic and optical modes. FMR experiments show that the Kittel curves of the two layers cannot be taken in isolation, but that their modelling needs to account for an interlayer exchange coupling. The angular dependence of FMR indicates a collective effect for the modes of the magnetically hard CoFe and soft NiFe layer. The XFMR precessional scans show that the acoustic mode is dominated by the Ni signal with the Co and Ni magnetization precessing in phase, whereas the optical mode is dominated by the Co signal with the Co and Ni magnetization precessing in anti-phase. The response of the Co signal at the Ni resonance, and vice versa, show induced changes in both amplitude and phase, which can be ascribed to the interface exchange coupling. An interesting aspect of phase-resolved XFMR is the ability to distinguish between static and dynamic exchange coupling. The element-specific precessional scans of the NiFe/CoFe bilayer clearly have the signature of static exchange coupling, in which the effective field in one layer is aligned along the magnetization direction of the other layer.

Journal Keywords: Absorption; Cobalt Compounds; Epitaxy; Ferromagnetic Resonance; Ghz Range; Iron Compounds; Layers; Magnetization; Nickel Compounds; Optical Modes; Signals; Simulation; Synchrotron Radiation; X Radiation

Subject Areas: Physics

Instruments: I06-Nanoscience , I10-Beamline for Advanced Dichroism

Other Facilities: Beamline PM3 (dipolePGMvariable polarization) at BESSY II of the Helmholtz-Zentrum Berlin.


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