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Investigations on the g factors of the ground and excited states for Cu2+ ions in ZnO crystal

机译:ZnO晶体中Cu2 +离子的基态和激发态g因子研究

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The g factors g// and g⊥ of the ground Γ_6(~2T_2) and excited Γ_(4,5)(~2E), Γ_6(~2E) states for trigonal Cu~(2+) centres in ZnO crystals are calculated from three theoretical methods, the complete diagonalization (of the energy matrix) method, the second-order perturbation method (PTM-I) and the simplified second-order perturbation method (PTM-II, this method was described in an earlier paper). These methods are based on the cluster approach in which the spin-orbit coupling parameters Χ, Χ' and the orbital reduction factors k, k' are calculated from a semi-empirical molecular orbital method. The crystal-field parameters used in the calculations are obtained from the superposition model and so the defect structure of Cu ~(2+) centres in ZnO can be acquired. The calculated g factors from the three methods are in reasonable agreement with the experimental values and the defect structure of Cu~(2+) centres in ZnO is acquired. It appears that in some cases the approximate PTM can be applied in the studies of g factors of various states. The conditions that the PTM are ineffective are discussed.
机译:计算出ZnO晶体中Cu〜(2+)中心的地面Γ_6(〜2T_2)和激发Γ_(4,5)(〜2E),Γ_6(〜2E)态的g因子g //和g⊥从三种理论方法来看,(能量矩阵的)完全对角化方法,二阶扰动方法(PTM-I)和简化的二阶扰动方法(PTM-II,此方法已在较早的论文中进行了描述)。这些方法基于聚类方法,在该聚类方法中,根据半经验分子轨道方法计算了自旋轨道耦合参数X,X'和轨道减小因子k,k'。从叠加模型中获得了计算中使用的晶体场参数,从而可以获得ZnO中Cu〜(2+)中心的缺陷结构。三种方法计算得到的g因子与实验值基本吻合,得到了ZnO中Cu〜(2+)中心的缺陷结构。似乎在某些情况下,可以将近似PTM应用于各种状态的g因子的研究。讨论了PTM无效的条件。

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