Abstract

Spin waves in ferrimagnetic yttrium iron garnet (YIG) films with ultralow magnetic damping are relevant for magnon-based spintronics and low-power wave-like computing. The excitation frequency of spin waves in YIG is rather low in weak external magnetic fields because of its small saturation magnetization, which limits the potential of YIG films for high-frequency applications. Here, we demonstrate how exchange-coupling to a CoFeB film enables efficient excitation of high-frequency perpendicular standing spin waves (PSSWs) in nanometer-thick (80 nm and 295 nm) YIG films using uniform microwave magnetic fields. In the 295-nm-thick YIG film, we measure intense PSSW modes up to 10th order. Strong hybridization between the PSSW modes and the ferromagnetic resonance mode of CoFeB leads to characteristic anti-crossing behavior in broadband spin-wave spectra. We explain the excitation of PSSWs by exchange coupling between forced magnetization precessions in the YIG and CoFeB layers. If the amplitudes of these precessions are different, a dynamic exchange torque is generated, causing the emission of spin waves from the interface. PSSWs form when the wave vector of the spin waves matches a perpendicular confinement condition. PSSWs are not excited if exchange coupling between YIG and CoFeB is eliminated by a 10 nm Ta spacer layer. Micromagnetic simulations confirm the exchange-torque-driven mechanism.

Highlights

  • Magnonics aims at the use of spin waves for the processing, storage, and transmission of information[1,2,3,4,5,6]

  • Used perpendicular standing spin waves (PSSWs) to extract the exchange constant[25] and Navabi et al demonstrated the excitation of a 1st order PSSW mode in a 100-nm-thick yttrium iron garnet (YIG) film on top of an undulating substrate[28]

  • We show that forced magnetization precessions in YIG and CoFeB, driven by an approximately uniform microwave magnetic field, induce a dynamic exchange torque at the interface when the precessions are dissimilar

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Summary

Results

At even higher frequency or magnetic bias field, the PSSWs move further away from the CoFeB FMR mode and relatively closer to the FMR mode in YIG Under these conditions, the forced magnetization precession in YIG is larger than in CoFeB and, a dynamic exchange torque is regenerated. We consider an excitation frequency of 4.5 GHz, in between the frequencies of the p = 3 and p = 4 PSSW modes (see Fig. 7a) Under these circumstances, spin waves are again emitted from the YIG/ CoFeB interface by the dynamic exchange torque. The application of an uniform microwave magnetic field produces a strong dynamic exchange torque at the YIG/CoFeB interface This situation is attained if the saturation magnetization is smaller in the PSSW-carrying film

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