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Na(2)V(3)O(7)中的电子结构和自旋交换相互作用:一种四价钒氧化物纳米管状相。

Electronic structure and spin exchange interactions in Na(2)V(3)O(7): a vanadium(IV) oxide nanotubular phase.

机构信息

Departament de Química Física i Inorgànica, Universitat Rovira i Virgili, Marcel.li Domingo s/n, 43007 Tarragona, Spain.

出版信息

Inorg Chem. 2009 Jul 6;48(13):5779-89. doi: 10.1021/ic900105u.

Abstract

The electronic structure of the inorganic nanotubular phase Na(2)V(3)O(7) has been studied by means of first-principles DFT calculations. The magnetic behavior in this system is relatively complex to study because there are as many as 30 different exchange interactions in the unit cell. The coupling constants are computed directly from the energy differences of several spin configurations. It is found that because of the special geometry of the nanotube, the nearest-neighbor coupling constants are not the only important ones and other next-nearest-neighbor constants cannot be neglected. In contrast with previous studies, it is found that at least 12 different coupling constants must be considered to correctly describe the spin arrangement in this system. However, to get more meaningful values for the smaller constants, a larger set of at least 17 constants must be explicitly taken into account. The lowest-energy collinear spin configuration is found to exhibit ferromagnetic coupling between the rings of the nanotube, whereas the coupling can be ferro- or antiferromagnetic within those rings. This leads to two important spin-frustrated interactions. Use of the so-called dimer approximation (i.e., substituting 16 paramagnetic V(IV) ions of the nanotube by 16 diamagnetic Ti(IV) ions, thus keeping the total charge of the system constant and leaving only two magnetic centers) is found to give invaluable hints concerning the nature of the magnetic interactions. This procedure may be helpful to analyze the magnetic properties of similar non-trivial systems with many paramagnetic centers.

摘要

采用第一性原理 DFT 计算研究了无机纳米管状相 Na(2)V(3)O(7)的电子结构。由于单元胞中存在多达 30 种不同的交换相互作用,因此该体系的磁行为研究起来比较复杂。通过计算几个自旋组态的能量差,直接得到了耦合常数。研究发现,由于纳米管的特殊几何形状,最近邻耦合常数并不是唯一重要的常数,其他次近邻常数也不能忽略。与之前的研究不同,发现至少需要考虑 12 个不同的耦合常数才能正确描述该体系中的自旋排列。然而,为了得到较小常数更有意义的值,必须明确考虑至少 17 个常数的更大集合。研究发现,最低能量的共线自旋组态表现出纳米管环之间的铁磁耦合,而环内的耦合可以是铁磁或反铁磁。这导致了两个重要的自旋受挫相互作用。采用所谓的二聚体近似(即,用纳米管中的 16 个顺磁 V(IV)离子代替 16 个抗磁 Ti(IV)离子,从而保持系统总电荷不变,只留下两个磁中心),发现这对于理解磁相互作用的性质有很大的帮助。该方法可能有助于分析具有许多顺磁中心的类似复杂体系的磁性质。

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