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Magnetic interactions in strongly correlated systems: spin and orbital contributions

机译:强相关系统中的磁相互作用:自旋和轨道   捐款

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摘要

We present a technique to map an electronic model with local interactions (ageneralized multi-orbital Hubbard model) onto an effective model of interactingclassical spins, by requiring that the thermodynamic potentials associated tospin rotations in the two systems are equivalent up to second order in therotation angles. This allows to determine the parameters of relativistic andnon-relativistic magnetic interactions in the effective spin model in terms ofequilibrium Green's functions of the electronic model. The Hamiltonian of theelectronic system includes, in addition to the non-relativistic part,relativistic single-particle terms such as the Zeeman coupling to an externalmagnetic fields, spin-orbit coupling, and arbitrary magnetic anisotropies; theorbital degrees of freedom of the electrons are explicitly taken into account.We determine the complete relativistic exchange tensors, accounting foranisotropic exchange, Dzyaloshinskii-Moriya interactions, as well as additionalnon-diagonal symmetric terms (which may include dipole-dipole interaction). Ourprocedure provides the complete exchange tensors in a unified framework,including previously disregarded features such as the vertices of two-particleGreen's functions and non-local self-energies. We do not assume any smallnessin spin-orbit coupling, so our treatment is in this sense exact. Finally, weshow how to distinguish and address separately the spin, orbital andspin-orbital contributions to magnetism.
机译:通过提出两个系统中与自旋旋转相关的热力学势能等价于旋转角度的二阶,我们提出了一种将具有局部相互作用的电子模型(经平均化的多轨道哈伯德模型)​​映射到相互作用的经典自旋的有效模型上的技术。这允许根据电子模型的平衡格林函数来确定有效自旋模型中相对论和非相对论磁相互作用的参数。电子系统的哈密顿量除非相对论部分外,还包括相对论单粒子术语,例如与外部磁场的塞曼耦合,自旋轨道耦合和任意磁各向异性。我们明确地确定了电子的轨道自由度。我们确定了完整的相对论交换张量,各向异性交换,Dzyaloshinskii-Moriya相互作用以及其他非对角对称项(可能包括偶极-偶极相互作用)。我们的过程在统一的框架中提供完整的交换张量,包括以前忽略的特征,例如,two-particleGreen函数的顶点和非局部自能。我们不认为自旋轨道耦合有任何小问题,因此在这种意义上我们的处理是精确的。最后,我们展示了如何区分和解决自旋,轨道和自旋轨道对磁性的贡献。

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