超越单粒子图像的Ni磁康普顿剖面:动态平均场理论的数值精确和微扰解算

A. James, M. Sekania, S. Dugdale, L. Chioncel
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引用次数: 5

摘要

我们利用密度泛函理论,辅以动态平均场理论(DMFT)处理的电子相关,计算了Ni的磁性康普顿剖面(MCPs)。我们提出了理论和实验mcp之间的比较。理论mcp分别用KKR法和全势线性增广平面波法计算,前者采用微扰自旋极化t矩阵波动交换近似DMFT求解器,后者采用数值精确的连续时间量子蒙特卡罗DMFT求解器。我们发现总磁矩随着原子内库仑斥力的减小而减小,这也反映在相应的mcp中。在实验测量中得到的总磁矩可以用中间值$U$再现。谱函数表明,相对于密度泛函理论计算,少数X$_2$费米表面袋收缩并变浅。
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Magnetic Compton profiles of Ni beyond the one-particle picture: Numerically exact and perturbative solvers of dynamical mean-field theory
We calculated the magnetic Compton profiles (MCPs) of Ni using density functional theory supplemented by electronic correlations treated within dynamical mean-field theory (DMFT). We present comparisons between the theoretical and experimental MCPs. The theoretical MCPs were calculated using the KKR method with the perturbative spin-polarized T-matrix fluctuation exchange approximation DMFT solver, as well as with the full potential linear augmented planewave method with the numerically exact continuous-time quantum Monte Carlo DMFT solver. We show that the total magnetic moment decreases with the intra-atomic Coulomb repulsion $U$, which is also reflected in the corresponding MCPs. The total magnetic moment obtained in experimental measurements can be reproduced by intermediate values of $U$. The spectral function reveals that the minority X$_2$ Fermi surface pocket shrinks and gets shallower with respect to the density functional theory calculations.
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