N. I. Gribova, V. N. Berzhansky, S. N. Polulyakh, V. I. Belotelov
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引用次数: 0
摘要
磁光法拉第效应是由透明磁性材料中的电偶极子和磁偶极子跃迁决定的。与此同时,反法拉第效应仍然用只包括电偶极子跃迁的表达式来描述。我们从理论上考虑了磁偶极子对反法拉第效应的贡献,并以铁氧体石榴石薄膜为例,得出了反法拉第效应在近红外范围内对波长的依赖性(磁偶极子的贡献在此变得显著)。研究表明,虽然对于均质薄膜,反法拉第效应的两种贡献都会发生,但对于具有周期性纳米结构的薄膜,在 TE 波导模式激发下,只有磁偶极子反法拉第效应才会表现出来,这可能有助于对其进行实验观察。
Inverse Faraday Effect in Ferrite–Garnet Films in the Near-Infrared Range
The magneto-optical Faraday effect is determined by the electric dipole and magnetic dipole transitions in a transparent magnetic material. At the same time, the inverse Faraday effect is still described by an expression that includes only electric dipole transitions. The magnetic dipole contribution to the inverse Faraday effect is considered theoretically, and the dependence of the inverse Faraday effect on the wavelength in the near-infrared range (where the magnetic dipole contribution becomes significant) is obtained by the example of a ferrite–garnet film. It is shown that, although both contributions to the inverse Faraday effect always take place for homogeneous films, only the magnetic-dipole inverse Faraday effect manifests itself for films with a periodic nanostructure upon excitation by a TE waveguide mode, which may be useful for its experimental observation.
期刊介绍:
All topics of experimental and theoretical physics including gravitation, field theory, elementary particles and nuclei, plasma, nonlinear phenomena, condensed matter, superconductivity, superfluidity, lasers, and surfaces.