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Electronic and Magnetic Structures, Magnetic Hyperfine Fields and Electric Field Gradients in UX3 (X = In, Tl, Pb) Intermetallic Compounds

机译:UX3(X = In,TL,PB)金属间化合物中的电子和磁性结构,磁性杂质场和电场梯度

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摘要

Cubic uranium compounds such as UX3 (X is a non-transition element of groups IIIA or IVA) exhibit highly diverse magnetic properties, including Pauli paramagnetism, spin fluctuation and anti-ferromagnetism. In the present paper, we explore the structural, electronic and magnetic properties as well as the hyperfine fields (HFFs) and electric field gradients (EFGs) with quadrupole coupling constant of UX3 (X = In, Tl, Pb) compounds using local density approximation, Perdew-Burke-Ernzerhof parametrization of generalized gradient approximation (PBE-GGA) including the Hubbard U parameter (GGA + U), a revised version of PBE-GGA that improves equilibrium properties of densely packed solids and their surfaces (PBEsol-GGA), and a hybrid functional (HF-PBEsol). The spin orbit-coupling calculations have been added to investigate the relativistic effect of electrons in these materials. The comparison between the experimental parameters and our calculated structural parameters we confirm the consistency and effectiveness of our theoretical tools. The computed magnetic moments show that magnetic moment increases from indium to lead in the UX3 family, and all these compounds are antiferromagnetic in nature. The EFGs and HFFs, as well as the quadrupole coupling constant of UX3 (X = In, Tl, Pb), are discussed in detail. These properties primarily originate from f and p states of uranium and post-transition sites.
机译:等级铀化合物如UX3(X是IIIA组或IVA的非过渡元件)表现出高度多样化的磁性,包括Pauli Paramagnetis,旋转波动和抗铁磁性。在本文中,我们使用局部密度近似探讨了具有UX3(X = In,TL,PB)化合物的四极耦合常数的结构,电子和磁性和电场(HFF)和电场梯度(EFG) ,包括Hubbard U参数(GGA-GGA)的广义梯度近似(PBE-GGA)的Perdew-Burke-Ernzerhof(PBE-GGA),PBE-GGA的修订版本,提高了密集填充固体的平衡性质及其表面(PBESOL-GGA)和杂交功能(HF-Pbesol)。已经添加了自旋轨道偶联计算以研究这些材料中电子的相对论效应。实验参数与我们计算的结构参数之间的比较我们确认了我们理论工具的一致性和有效性。计算的磁矩表明,磁矩从UX3家族中的铟增加,并且所有这些化合物都是反铁磁性的。详细讨论了EFGS和HFFS,以及UX3(X = In,TL,PB)的四极耦合常数。这些性质主要来自F和P铀和过渡后位点的F和P状态。

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