2016
DOI: 10.1103/physrevb.93.140404
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Current control of magnetic anisotropy via stress in a ferromagnetic metal waveguide

Abstract: We demonstrate that in-plane charge current can effectively control the spin precession resonance in an Al2O3/CoFeB/Ta heterostructure. Brillouin Light Scattering (BLS) was used to detect the ferromagnetic resonance field under microwave excitation of spin waves at fixed frequencies. The current control of spin precession resonance originates from modification of the in-plane uniaxial magnetic anisotropy field k , which changes symmetrically with respect to the current direction. Numerical simulation suggests … Show more

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Cited by 7 publications
(4 citation statements)
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“…One conclusion that can be drawn from Table II is case of the present study. The resulting uniaxial stress produces a magnetic anisotropy field H K which affects spin precession resonance frequencies [37] and also can account for the apparent temperature-dependent shift in the mobility cures shown in Fig. 11.…”
Section: Experimental Evidence For the Simulated Dw Behaviormentioning
confidence: 97%
“…One conclusion that can be drawn from Table II is case of the present study. The resulting uniaxial stress produces a magnetic anisotropy field H K which affects spin precession resonance frequencies [37] and also can account for the apparent temperature-dependent shift in the mobility cures shown in Fig. 11.…”
Section: Experimental Evidence For the Simulated Dw Behaviormentioning
confidence: 97%
“…Namely, the magnitude of the PMA should be inversely proportional to the amplitude of the current in the microcoil. Besides, the PMA may also be affected by a thermal stress, 42 which could be caused by the thermal expansion of the sample due to the heating effect. In Supporting Information Note 1, we show experimental evidence that the variation of the PMA is dominated by thermalization, while the effect of stress is not significant compared to that induced by the thermal effect.…”
Section: T H Imentioning
confidence: 99%
“…The misfit strains u xx and u yy are expected to be fully relaxed at the growth temperature T g = 573 K, which is well above the Curie temperature T C = 393 K of BaTiO 3 . On cooling from T g , nonzero strains appear in the film owing to the difference in the thermal expansion coefficients of paraelectric BaTiO 3 , α 0 = 10 × 10 6 K −1 [42], and Co 40 Fe 40 B 20 , α b = 12 × 10 6 K −1 [43]. Taking into account the fact that spontaneous strains appear in BaTiO 3 below T C , we obtain…”
Section: A Magnetic Anisotropy Of the Co 40 Fe 40 B 20 /Batio 3 Hetementioning
confidence: 99%