Thickness dependence of spin pumping at YIG/Pt interface
Tomoya Tashiro, Ryo Takahashi, Y. Kajiwara, Kazuya Ando, Hiroyasu Nakayama, Takashi Yoshino, Daisuke Kikuchi, Eiji Saitoh
Abstract
Tomoya Tashiro, Ryo Takahashi, Y. Kajiwara, Kazuya Ando, Hiroyasu Nakayama, Takashi Yoshino, Daisuke Kikuchi, Eiji Saitoh
Abstract
ABSTRACT We report Y 3 Fe 5 O 12 thickness dependence of spin pumping, spin current generation from magnetization dynamics, in magnetic insulator Y 3 Fe 5 O 12 /metal Pt bilayer films. We prepared different thickness Y 3 Fe 5 O 12 films by the metal-organic decomposition method and measured the electromotive force due to the inverse spin Hall effect induced by the spin pumping in Y 3 Fe 5 O 12 /Pt films. We found that spin-mixing conductance, or spin-pumping efficiency, Y 3 Fe 5 O 12 /Pt films constant for the di fferent thickness is almost same in various Y 3 Fe 5 O 12 thickness. This result is consistent with the prediction of the spin pumping; the spin-pumping efficiency is determined by the exchange interaction at the Y 3 Fe 5 O 12 /Pt interface. Keywords: Spintronics, Spin pumping, Spin current, Inverse spin Hall effect 1. INTRODUCTION There has been great interest in the field of spintronics [1]-[37], which is a new device technology for efficient magnetic memories and computing devices base d on electron spins. In this field, the generation and detection of a spin current [1]-[4], [7]-[11], [15], [16], [27]-[33], [35], [36], a flow of spin angular momentum in a solid, plays an important role. One method for generating spin currents is the spin pumping [5], [6], [12]-[14], [17]-[26], [34], [37]. The spin pumping generates a spin current from magnetization precession driven by the ferromagnetic resonance (FMR) or spin-wave resonance at ferro(ferri)magnetic/paramagnetic interfaces. The strength of the spin pumping is proportional to the spin-mixing conductance [20], [26]. Recently, spin pumping was observed at ferrimagnetic insulator Y
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ABSTRACT We report Y 3 Fe 5 O 12 thickness dependence of spin pumping, spin current generation from magnetization dynamics, in magnetic insulator Y 3 Fe 5 O 12 /metal Pt bilayer films. We prepared different thickness Y 3 Fe 5 O 12 films by the metal-organic decomposition method and measured the electromotive force due to the inverse spin Hall effect induced by the spin pumping in Y 3 Fe 5 O 12 /Pt films. We found that spin-mixing conductance, or spin-pumping efficiency, Y 3 Fe 5 O 12 /Pt films constant for the di fferent thickness is almost same in various Y 3 Fe 5 O 12 thickness. This result is consistent with the prediction of the spin pumping; the spin-pumping efficiency is determined by the exchange interaction at the Y 3 Fe 5 O 12 /Pt interface. Keywords: Spintronics, Spin pumping, Spin current, Inverse spin Hall effect 1. INTRODUCTION There has been great interest in the field of spintronics [1]-[37], which is a new device technology for efficient magnetic memories and computing devices base d on electron spins. In this field, the generation and detection of a spin current [1]-[4], [7]-[11], [15], [16], [27]-[33], [35], [36], a flow of spin angular momentum in a solid, plays an important role. One method for generating spin currents is the spin pumping [5], [6], [12]-[14], [17]-[26], [34], [37]. The spin pumping generates a spin current from magnetization precession driven by the ferromagnetic resonance (FMR) or spin-wave resonance at ferro(ferri)magnetic/paramagnetic interfaces. The strength of the spin pumping is proportional to the spin-mixing conductance [20], [26]. Recently, spin pumping was observed at ferrimagnetic insulator Y
Key concepts: Spin pumping, Spintronics, Spin Hall effect, Condensed matter physics, Ferromagnetic resonance, Spin diffusion, Spin (aerodynamics), Magnetization