相干磁振子的和频激发

D. M. Juraschek, Derek S. Wang, P. Narang
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引用次数: 17

摘要

磁振子的相干激发通常是通过拉曼散射过程来实现的,在拉曼散射过程中,驱动场的差频分量与磁振子能量共振。在这里,我们描述了驱动场的和频分量可以通过双粒子吸收过程相干激发磁振子的机制。我们使用Landau-Lifshitz-Gilbert形式比较了反铁磁模型系统中不同类型的脉冲受激和离子拉曼散射过程及其和频率对应过程诱导的自旋进动振幅。我们表明,由线性极化驱动场启用的和频机制产生的激发效率与现有的拉曼技术相当或更高,而椭圆偏振只产生弱偏振和圆偏振,根本没有和频分量。本文提出的机制完成了利用拉曼型过程进行动态自旋控制的图谱。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Sum-frequency excitation of coherent magnons
Coherent excitation of magnons is conventionally achieved through Raman scattering processes, in which the difference-frequency components of the driving field are resonant with the magnon energy. Here, we describe mechanisms by which the sum-frequency components of the driving field can be used to coherently excite magnons through two-particle absorption processes. We use the Landau-Lifshitz-Gilbert formalism to compare the spin-precession amplitudes that different types of impulsive stimulated and ionic Raman scattering processes and their sum-frequency counterparts induce in an antiferromagnetic model system. We show that sum-frequency mechanisms enabled by linearly polarized driving fields yield excitation efficiencies comparable or larger than established Raman techniques, while elliptical polarizations produce only weak and circularly polarizations no sum-frequency components at all. The mechanisms presented here complete the map for dynamical spin control by the means of Raman-type processes.
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