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纳米级铁磁波导中的自旋钉扎与自旋波色散

Spin Pinning and Spin-Wave Dispersion in Nanoscopic Ferromagnetic Waveguides.

作者信息

Wang Q, Heinz B, Verba R, Kewenig M, Pirro P, Schneider M, Meyer T, Lägel B, Dubs C, Brächer T, Chumak A V

机构信息

Fachbereich Physik and Landesforschungszentrum OPTIMAS, Technische Universität Kaiserslautern, D-67663 Kaiserslautern, Germany.

Graduate School Materials Science in Mainz, Staudingerweg 9, 55128 Mainz, Germany.

出版信息

Phys Rev Lett. 2019 Jun 21;122(24):247202. doi: 10.1103/PhysRevLett.122.247202.

Abstract

Spin waves are investigated in yttrium iron garnet waveguides with a thickness of 39 nm and widths ranging down to 50 nm, i.e., with an aspect ratio thickness over width approaching unity, using Brillouin light scattering spectroscopy. The experimental results are verified by a semianalytical theory and micromagnetic simulations. A critical width is found, below which the exchange interaction suppresses the dipolar pinning phenomenon. This changes the quantization criterion for the spin-wave eigenmodes and results in a pronounced modification of the spin-wave characteristics. The presented semianalytical theory allows for the calculation of spin-wave mode profiles and dispersion relations in nanostructures.

摘要

利用布里渊光散射光谱对厚度为39纳米、宽度低至50纳米(即厚度与宽度的纵横比接近1)的钇铁石榴石波导中的自旋波进行了研究。实验结果通过半解析理论和微磁模拟得到了验证。发现了一个临界宽度,低于该宽度时,交换相互作用会抑制偶极钉扎现象。这改变了自旋波本征模的量子化准则,并导致自旋波特性发生显著改变。所提出的半解析理论可用于计算纳米结构中的自旋波模式轮廓和色散关系。

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