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引用次数: 0
摘要
我们对非共轭反铁磁体(AFMs)、Mn3Ir 和 Mn3Sn 的 X 射线磁圆二色性光谱(XMCD)进行了第一原理研究。通过计算自旋、轨道和磁偶极矩的投影态密度,我们评估了 AFM 的 XMCD 光谱。我们发现,自旋磁矩的贡献几乎消失,而磁偶极矩的贡献则给出了有限的 XMCD 光谱。这表明这些原子力显微镜是研究源于磁偶极矩的 XMCD 光谱的理想系统。通过分析有自旋轨道耦合和无自旋轨道耦合的磁对称性,我们得出结论:在无自旋轨道耦合的情况下,确保自旋磁矩抵消的对称操作对这一特征至关重要。我们还发现,锰 3d 轨道的自旋轨道耦合对 XMCD 光谱的形状影响很小。
X-ray Magnetic Circular Dichroism Arising from the Magnetic Dipole Moment in Antiferromagnets
We present a first-principles study of the X-ray magnetic circular dichroism (XMCD) spectra for noncollinear antiferromagnets (AFMs), Mn3Ir and Mn3Sn. By calculating the projected density of states for spin, orbital, and magnetic dipole moments, we evaluated the XMCD spectra for the AFMs. We found that the contributions of the spin magnetic moment almost vanish while those from the magnetic dipole moments give finite XMCD spectra. This indicates that these AFMs are ideal systems to study the XMCD spectra originating from the magnetic dipole moment. By analyzing the magnetic symmetry with and without spin–orbit couplings, we concluded that a symmetry operation that assures a cancellation of spin magnetic moments in the case without spin–orbit couplings is crucial for this feature. We also showed that the spin–orbit couplings for the Mn 3d orbitals have little effect on the shape of the XMCD spectra.
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