首页> 外文期刊>Journal of Physics. Condensed Matter >Using density functional theory to describe slowly varying fluctuations at finite temperatures: local magnetic moments in Gd and the 'not so local' moments of Ni
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Using density functional theory to describe slowly varying fluctuations at finite temperatures: local magnetic moments in Gd and the 'not so local' moments of Ni

机译:使用密度泛函理论描述在有限温度下缓慢变化的波动:Gd中的局部磁矩和Ni的“非局部”矩

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摘要

We briefly describe the density functional theory (DFT)-based 'disordered local moment' (DLM) picture for magnetism at finite temperatures. It shows how relatively slowly fluctuating local moments can emerge from the interacting electrons of many materials. Such entities have rigid magnitudes and fluctuate their orientations from atomic site to atomic site on a timescale long compared to other electronic times. We illustrate this theory with calculations of the magnetocaloric effect in Gd where we find excellent agreement with experiments. Fluctuating moments do not appear to establish naturally over such small regions for some other materials. We show how the DFT-DLM theory can be extended to these materials with the use of the Korringa-Kohn-Rostoker nonlocal coherent potential approximation (KKR-NLCPA) to allow for more extensive, slow magnetic fluctuations. We present the first application of this approach by revisiting the description of the magnetic fluctuations prevalent in the paramagnetic state of nickel. We find that local moments can emerge above T_c and that these form coherently over small clumps of atomic sites (4-8 sites).
机译:我们简要描述了在有限温度下基于密度泛函理论(DFT)的“无序局部矩”(DLM)图像。它显示了许多材料相互作用的电子如何相对缓慢地波动局部矩。与其他电子时间相比,这样的实体具有严格的强度,并且在一个时间尺度上从一个原子位置到另一个原子位置的取向波动很大。我们通过计算Gd中的磁热效应来说明这一理论,我们发现该理论与实验非常吻合。对于某些其他材料,在如此小的区域上似乎不会自然地建立起波动的力矩。我们展示了如何使用Korringa-Kohn-Rostoker非局部相干势能近似(KKR-NLCPA)来将DFT-DLM理论扩展到这些材料,以允许更广泛的缓慢磁波动。通过重新介绍在顺磁性状态下普遍存在的磁波动的描述,我们介绍了该方法的首次应用。我们发现局部矩可以出现在T_c之上,并且它们在小块的原子位点(4-8个位点)上连贯地形成。

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