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N 掺杂在诱导(ZnO)n 团簇(n = 1-16)中产生铁磁性中的作用。

The role of N dopant in inducing ferromagnetism in (ZnO)n clusters (n = 1-16).

机构信息

Department of Physics, Center of Advanced Studies in Physics, Panjab University, Chandigarh-160014, India.

出版信息

J Phys Condens Matter. 2011 Nov 9;23(44):446006. doi: 10.1088/0953-8984/23/44/446006.

Abstract

The effect of nitrogen doping on the magnetic properties of (ZnO)(n) clusters (n = 1-16) has been investigated using spin polarized density functional theory. The total energy calculations suggest that N is more stable at the O site than at the Zn site in (ZnO)(n) clusters and induces a magnetic moment of 1 μ(B)/N atom. The N-Zn-N configuration is more stable than isolated N for 3D structures. The N dopants do not show any tendency for clustering. The binding energy is found to decrease with the increase in the number of N dopants. The magnetic moment increases gradually with the increase in the number of atoms with 1 μ(B)/N atom for n ≤ 4 and less than 1 μ(B)/N for n > 4. The local magnetic moment is mainly localized at the N site with a small magnetic moment induced at the O site. The presence of a Zn vacancy (V(Zn)) induced an additional magnetic moment of 2 μ(B) on the nearest O atoms. The N dopant prefers to form a N-V(Zn) pair. The combination of N and V(Zn) in 3D structures leads to a total magnetic moment of 3 μB. The Mulliken charge transfers from Zn to N and O in all N doped (ZnO)(n) clusters. The calculated results are consistent with existing experimental and theoretical results.

摘要

采用自旋极化密度泛函理论研究了氮掺杂对(ZnO)(n)团簇(n=1-16)磁性能的影响。总能量计算表明,在(ZnO)(n)团簇中,N 比在 Zn 位更稳定,并且诱导 1 μ(B)/N 原子的磁矩。对于 3D 结构,N-Zn-N 构型比孤立 N 更稳定。N 掺杂剂没有表现出任何聚类趋势。随着 N 掺杂剂数量的增加,结合能减小。磁矩随着原子数量的增加而逐渐增加,对于 n≤4,每个 N 原子的磁矩为 1 μ(B),对于 n>4,每个 N 原子的磁矩小于 1 μ(B)。局域磁矩主要定域在 N 位,在 O 位诱导出较小的磁矩。Zn 空位(V(Zn))的存在在最近的 O 原子上诱导了 2 μ(B)的附加磁矩。N 掺杂剂倾向于形成 N-V(Zn)对。在 3D 结构中,N 和 V(Zn)的组合导致总磁矩为 3 μB。在所有 N 掺杂的(ZnO)(n)团簇中,Mulliken 电荷从 Zn 转移到 N 和 O。计算结果与现有的实验和理论结果一致。

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