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Unconstrained magnetism in nanostructures at zero temperature: An ultimate goal

机译:零温度下纳米结构中的无约束磁性:最终目标

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摘要

Recent calculations have shown that the magnetization of nanostructures cannot be safely described by collinear models based on phenomenological Ising Hamiltonian or electronic structure approaches. When interactions between spins are screened by electronic clouds, a Heisenberg Hamiltonian presents a safe approach for ground state calculations as well as for the determination of temperature dependant magnetization. In metallic systems, due to strong interactions between spins, semi-empirical models like Extended Huckel, tight-binding or Periodic Anderson Model (PAM) have been used. Within these oversimplified approaches, vector magnetization could be tested and, for nanostructures, it generally led to non-collinear ground states. Ab initio calculations based on Kohn-Sham techniques can also describe non-collinear ground states but, because these techniques work in k-space, periodicity is necessary. This is a strong approximation for nanostructures. Therefore, in the present short review, we essentially focus on non-collinear magnetism of nanostructures by means of PAM approaches.
机译:最近的计算表明,基于现象学伊辛·哈密顿量或电子结构方法的共线模型不能安全地描述纳米结构的磁化强度。当电子云屏蔽了自旋之间的相互作用时,海森堡哈密顿量为基态计算以及与温度相关的磁化强度的确定提供了一种安全的方法。在金属系统中,由于自旋之间的强烈相互作用,因此使用了半经验模型,例如扩展Huckel,紧束缚或周期安德森模型(PAM)。在这些过于简化的方法中,可以测试矢量磁化强度,并且对于纳米结构,通常会导致非共线基态。基于Kohn-Sham技术的从头计算也可以描述非共线基态,但是,由于这些技术在k空间中起作用,因此周期性是必需的。这是对纳米结构的强近似。因此,在本篇简短的综述中,我们主要通过PAM方法研究纳米结构的非共线磁性。

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