2014
DOI: 10.1103/physrevb.89.140405
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Control of propagating spin waves via spin transfer torque in a metallic bilayer waveguide

Abstract: We investigate the effect of a direct current on propagating spin waves in a CoFeB/Ta bilayer structure. Using the micro-Brillouin light scattering technique, we observe that the spin wave damping and amplitude may be attenuated or amplified depending on the direction of the current and the applied magnetic field. Our work suggests an effective approach for electrically controlling the propagation of spin waves in a magnetic waveguide and may be useful in a number of applications such as phase locked nano-osci… Show more

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Cited by 60 publications
(48 citation statements)
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“…The damping of the fundamental mode could be completely compensated by the SOT, and coherent auto‐oscillation was achieved . Tuning of the spin‐wave damping and SOT‐induced auto‐oscillation has also been achieved in ferromagnetic metallic multilayers Ta/CoFeB and Pt/NiFe …”
Section: Manipulation Of Magnetic Materials By Spin–orbit Torquesmentioning
confidence: 89%
“…The damping of the fundamental mode could be completely compensated by the SOT, and coherent auto‐oscillation was achieved . Tuning of the spin‐wave damping and SOT‐induced auto‐oscillation has also been achieved in ferromagnetic metallic multilayers Ta/CoFeB and Pt/NiFe …”
Section: Manipulation Of Magnetic Materials By Spin–orbit Torquesmentioning
confidence: 89%
“…In the context of a phase-conserving, mode-and frequency-selective amplification of traveling spin waves, the process of parallel pumping has, so far, proven superior to other approaches of spin-wave amplification, such as the reduction of the spin-wave damping by spin transfer torque (STT) [24][25][26][27]. Parallel pumping, or parallel parametric amplification, results from the interaction of selected spin waves with a sufficiently large dynamic effective magnetic field, which acts in parallel to the static magnetization and features two times the frequency of these spin waves.…”
Section: Introductionmentioning
confidence: 99%
“…The Curie temperatures of these materials are 560 K for YIG, and 550K to 870K for Py depending on the crystal structure 20,21 . BLS spectra are collected using a µBLS system, briefly described as follows 12,19,22 . A single frequency, linearly polarized 532 nm laser beam, normally incident on the sample, is focused using an objective lens (NA 0.70) to a spot size of approximately 1 µm in diameter.…”
mentioning
confidence: 99%