2011
DOI: 10.1103/physrevlett.107.146602
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Control of Spin Waves in a Thin Film Ferromagnetic Insulator through Interfacial Spin Scattering

Abstract: Control of spin waves in a ferrite thin film via interfacial spin scattering was demonstrated. The experiments used a 4.6  μm-thick yttrium iron garnet (YIG) film strip with a 20-nm thick Pt capping layer. A dc current pulse was applied to the Pt layer and produced a spin current across the Pt thickness. As the spin current scatters off the YIG surface, it can either amplify or attenuate spin-wave pulses that travel in the YIG strip, depending on the current or field configuration. The spin scattering also aff… Show more

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Cited by 129 publications
(105 citation statements)
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“…The enhanced Gilbert damping of all higher transverse modes is exactly twice that of the macrospin mode. In the dipole-exchange regime, for intermediate values of QL, the dipolar interaction causes a small asymmetry in the eigenvectors for positive and negative eigenfrequencies because modes traveling in opposite directions have different magnitudes of precession near the FI/NM interface [26], and spin-pumping from these modes therefore differ. This phenomenon also explains why the enhanced damping, ∆α, splits into different branches in this regime, as shown in Fig.…”
mentioning
confidence: 99%
“…The enhanced Gilbert damping of all higher transverse modes is exactly twice that of the macrospin mode. In the dipole-exchange regime, for intermediate values of QL, the dipolar interaction causes a small asymmetry in the eigenvectors for positive and negative eigenfrequencies because modes traveling in opposite directions have different magnitudes of precession near the FI/NM interface [26], and spin-pumping from these modes therefore differ. This phenomenon also explains why the enhanced damping, ∆α, splits into different branches in this regime, as shown in Fig.…”
mentioning
confidence: 99%
“…1(c)]. By applying a current between the electrodes, a spin current is locally injected into the [Co/Ni] layer due to a combination of the spin Hall effect in Pt [5][6][7] and Rashba effect at the Pt/[Co/Ni] interface [8,9], resulting in magnetization auto-oscillation. We label our device the spin current auto-oscillator (SCAO).…”
mentioning
confidence: 99%
“…The possibility to induce dynamical states of nanomagnets or change their static configuration by the currentinduced spin torque (ST) [1, 2] has stimulated intense research into current-induced phenomena in magnetic systems. While the early experiments utilized spin-polarized electric currents in magnetic multilayers [3,4], recent studies focused on the effects of spin current produced due to the spin-orbit interaction (SOI) in bilayers of ferromagnets (F) with heavy nonmagnetic metals (N) [5][6][7][8]. The spin-orbit effects that contribute to the currentinduced phenomena include the spin Hall effect (SHE) originating from SOI in N, the Rashba effect [9] and the Dzyaloshinskii-Moriya interaction (DMI) [10], both originating from the broken inversion symmetry at the F/N interface.…”
mentioning
confidence: 99%
“…This spin-Hall torque can counteract damping in the ferromagnet and has been shown to switch uniform magnetization, 6-9 drive domain walls, [10][11][12] and control precessional magnetization dynamics. 7,9,[13][14][15][16][17][18][19][20][21][22][23] Despite the demonstrated utility of the spin Hall effect, there exists a wide disparity in its reported magnitude parameterized by the spin Hall angle. For example, reported spin…”
mentioning
confidence: 99%