论文标题

电子相关性,旋转​​轨道耦合和cu中心的结构效应的相互作用,在quasi-two-two-dimensional磁铁中incu $ _ {2/3} $ v $ _ {1/3} $ _3 $ _3 $

Interplay of electron correlations, spin-orbit couplings, and structural effects for Cu centers in the quasi-two-dimensional magnet InCu$_{2/3}$V$_{1/3}$O$_3$

论文作者

Murugesan, R., Eldeeb, M. S., Yehia, M., Büchner, B., Kataev, V., Janson, O., Hozoi, L.

论文摘要

过渡金属中心的不常见配体配位通常与特殊的价壳电子构型和出色的物理特性有关。一个例子是带有线性协调的Fe $^+$离子,在单分子磁性研究领域进行了积极研究。 Here we address the nature of 3$d^9$ states for Cu$^{2+}$ ions sitting in the center of trigonal bipyramidal ligand cages in the quasi-two-dimensional honeycomb compound InCu$_{2/3}$V$_{1/3}$O$_3$, whose unusual magnetic properties were intensively studied in the recent past.特别是,我们讨论了该材料中结构效应,电子相关性和自旋轨道耦合的相互作用。相关的计算发现是与现有的电子结构模型相比,Cu($ xz $,$ yz $)和($ xy $,$ x^2 \!y^2 $)的序列不同,这对各种激发光谱的解释具有影响。一阶和二阶的自旋轨道相互作用比以前假设要强,这表明对于3 $ d^9 $配置的原理也可以实现相当丰富的单人离子磁性特性,可以通过正确调整这种较不常见的配体配位来适当调整晶体场状态的顺序。

Less common ligand coordination of transition-metal centers is often associated with peculiar valence-shell electron configurations and outstanding physical properties. One example is the Fe$^+$ ion with linear coordination, actively investigated in the research area of single-molecule magnetism. Here we address the nature of 3$d^9$ states for Cu$^{2+}$ ions sitting in the center of trigonal bipyramidal ligand cages in the quasi-two-dimensional honeycomb compound InCu$_{2/3}$V$_{1/3}$O$_3$, whose unusual magnetic properties were intensively studied in the recent past. In particular, we discuss the interplay of structural effects, electron correlations, and spin-orbit couplings in this material. A relevant computational finding is a different sequence of the Cu ($xz$, $yz$) and ($xy$, $x^2\!-\!y^2$) levels as compared to existing electronic-structure models, which has implications for the interpretation of various excitation spectra. Spin-orbit interactions, both first- and second-order, turn out to be stronger than previously assumed, suggesting that rather rich single-ion magnetic properties can be in principle achieved also for the 3$d^9$ configuration by properly adjusting the sequence of crystal-field states for such less usual ligand coordination.

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