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极性 altermagnet 候选材料 Mn2Mo3O8 中太赫兹模式的磁圆二色性及拉曼活性光频声子的选择规则

Magnetic circular dichroism of THz modes and selection rules of Raman-active optical phonons in the polar altermagnet candidate \ce{Mn2Mo3O8}

F. Schilberth, K. Vasin, M. Knauft, M. Kondákor, M. Vuckovic, N. Herrmann, K. Penc, M. Minola, B. Keimer, V. A. Martinez, K. Panda, A. A. Sirenko, L. Prodan, V. Tsurkan, A. A. Tsirlin, I. Kézsmárki, J. Deisenhofer

arXiv 2608.01062首次发表:更新:

AI 中文总结

研究 Mn2Mo3O8 的磁与振动激发,结合实验与从头算识别光频声子,发现磁有序态太赫兹带的磁圆二色性在4T自旋翻转跃迁以上消失,未观测到E2声子预期分裂。

AI 中文摘要

我们通过温度依赖拉曼散射和磁光太赫兹时域透射光谱,研究了共线 altermagnet 候选材料 Mn2Mo3O8 的磁激发与振动激发。通过与准确捕获振动本征模本征频率的从头算(ab initio)计算对比,我们识别出所有光频声子,包括此前拉曼研究中未发现的最低能量 A1 和 E2 型拉曼模式。此外,我们对比了 Mn2Mo3O8 的顺磁相和磁有序相中光活性声子的选择规则,并分析了关于伪角动量守恒的拉曼选择规则。未观测到预期的简并顺磁 E2 光频声子在磁有序时分裂为具有圆偏振模式的证据,这可能是由于 Mn2+ 典型的弱自旋轨道耦合。相反,我们在磁有序态中观测到宽太赫兹激发带处存在强磁圆二色性,该带可能源于双磁振子激发,仅具有电偶极活性,且具有依赖磁场的双组分精细结构,其磁圆二色性在 4 T 的自旋翻转跃迁以上消失。

英文摘要

We investigated the magnetic and vibrational excitations in the collinear altermagnet candidate \ce{Mn2Mo3O8} by temperature dependent Raman scattering and magneto-optical THz time-domain transmission spectroscopy. By comparison to \textit{ab initio} calculations accurately capturing the eigenfrequencies of the vibrational eigenmodes, we identify all optical phonons, including the lowest-lying Raman modes of $A_1$ and $E_2$ type, which had remained elusive in a previous Raman study. Moreover, we compare the selection rules for optically active phonons in the paramagnetic and the magnetically ordered phases of \ce{Mn2Mo3O8} and analyze the Raman selection rules with respect to pseudo-angular momentum conservation. No evidence of the expected splitting of the degenerate paramagnetic $E_2$ optical phonons into modes with circular polarization upon magnetic ordering could be resolved, likely due to weak spin-orbit coupling typical for Mn$^{2+}$. In contrast, we observe strong magnetic circular dichroism at a broad THz excitation band, emerging in the magnetically ordered state. This band, potentially originating from two-magnon excitations, is only electric-dipole active and features a field-dependent two-component fine structure. Its magnetic circular dichroism vanishes above the spin-flop transition at 4~T.

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