Role of material-dependent properties in THz field-derivative-torque-induced nonlinear magnetization dynamics

Arpita Dutta, Pratyay Mukherjee, Swosti P. Sarangi, Somasree Bhattacharjee, Shovon Pal, Ritwik Mondal
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Abstract

The traditional Landau-Lifshitz-Gilbert (LLG) equation has often delineated the linear and nonlinear magnetization dynamics, even at ultrashort timescales e.g., femtoseconds. In contrast, several other non-relativistic and relativistic spin torques have been reported as an extension of the LLG spin dynamics. Here, we explore the contribution of the relativistic field-derivative torque (FDT) in the nonlinear THz magnetization dynamics response applied to ferrimagnets with high Gilbert damping and exchange magnon frequency. Our findings suggest that the FDT plays a significant role in magnetization dynamics in both linear and nonlinear regimes, bridging the gap between the traditional LLG spin dynamics and experimental observations. We find that the coherent THz magnon excitation amplitude is enhanced with the field-derivative torque. Furthermore, a phase shift in the magnon oscillation is induced by the FDT term. This phase shift is almost 90 for the antiferromagnet, while it is almost zero for the ferrimagnet under our investigation. Analyzing the dual THz excitation and their FDT, we find that the nonlinear signals can not be distinctly observed without the FDT terms. However, the inclusion of the FDT terms produces distinct nonlinear signals which matches extremely well with the previously reported experimental results.
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材料特性在太赫兹场衍生力矩诱导非线性磁化动力学中的作用
传统的兰道-利夫希茨-吉尔伯特(LLG)方程经常描述线性和非线性磁化动力学,甚至在超短时间尺度(如飞秒)上也是如此。相比之下,作为 LLG 自旋动力学的扩展,其他一些非相对论和相对论自旋力矩也得到了报道。在这里,我们探讨了相对论场衍生力矩(FDT)在应用于具有高吉尔伯特阻尼和交换磁子频率的铁氧体磁体的非线性 THz 磁化动力学响应中的贡献。我们的研究结果表明,FDT 在线性和非线性磁化动力学中都发挥了重要作用,弥补了传统 LLG 自旋动力学与实验观察之间的差距。我们发现,相干太赫兹磁子激发振幅会随场衍生力矩而增强。此外,磁子振荡的相移是由 FDT 项引起的。这种相移在铁磁体中几乎为 90,而在我们研究的铁磁体中几乎为零。通过分析双重太赫兹激励及其 FDT,我们发现如果不加入 FDT 项,非线性信号就无法被明显观测到。
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