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Topology of the Spin-Polarized Charge Density in bcc and fcc Iron

机译:bcc和fcc铁中自旋极化电荷密度的拓扑

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We report the first investigation of the topology of spin-polarized charge density, specifically in bcc and fcc iron. While the total spin-density is found to possess the topology of the non-magnetic prototypical structures, the spin-polarized charge densities of bcc and high-spin fcc iron are atypical. In these cases, the two spin densities are correlated: the spin-minority electrons have directional bond paths and deep minima, while the spin-majority electrons fill these holes, reducing bond directionality. The presence of distinct spin topologies allows us to show that the two phase changes seen in fcc iron (paramagnetic to low-spin and low-spin to high-spin) are different. The former follows the Landau symmetry-breaking paradigm and proceeds without a topological transformation, while the latter involves a topological catastrophe.
机译:我们报告了自旋极化电荷密度的拓扑结构的首次调查,特别是在bcc和fcc铁中。虽然发现总自旋密度具有非磁性原型结构的拓扑,但bcc和高自旋fcc铁的自旋极化电荷密度却是非典型的。在这些情况下,两个自旋密度是相关的:自旋少数电子具有定向键路径和极小的深度,而自旋多数电子填充这些孔,从而降低了键的定向性。独特的自旋拓扑结构的存在使我们能够证明,在fcc铁中看到的两个相变(顺磁性到低旋转以及低旋转到高旋转)是不同的。前者遵循Landau破坏对称的范式,并且继续进行拓扑转换,而后者则涉及拓扑灾难。

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