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Handling Magnetic Coupling in Trinuclear Cu(II) Complexes

机译:处理三核Cu(II)配合物中的磁耦合

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The problem of deriving three different two-body magnetic couplings in three electrons/three centers in a general geometric arrangement is investigated using the trinudear Cu(II) HAKKEJ complex as a real case example. In these systems, one quartet and two doublet low lying electronic states exist, which define the magnetic spectra. However, the two possible linearly independent energy differences do not provide enough information to extract the three magnetic coupling constants. Here, we show how to obtain these parameters without making any assumption on the symmetry of the system from a combination of density functional- and wave function-based calculations. The density functional calculations explore various broken symmetry solutions and relate the corresponding energy to the expectation value of the Heisenberg Hamiltonian. This allows one to obtain all magnetic couplings, although their magnitude strongly depends on the exchange correlation functional. Interestingly, a constant ratio between the magnetic coupling constants along a series of investigated fimctionals is found. This provides an additional equation to be used when relying on energy differences between spin states, which in turn allow solving the Heisenberg spectrum. The magnetic couplings thus obtained are compared to the experiment. Implications for the appropriate interpretation of the experiment and for the study of more complex systems are discussed.
机译:以三核Cu(II)HAKKEJ络合物为实例,研究了在一般的几何排列中在三个电子/三个中心形成三个不同的两体磁耦合的问题。在这些系统中,存在一个四重态和两个双重态的低电子态,它们定义了电磁频谱。但是,两个可能的线性独立的能量差不能提供足够的信息来提取三个磁耦合常数。在这里,我们展示了如何在不基于密度函数和基于波动函数的计算组合中对系统对称性做出任何假设的情况下获得这些参数。密度泛函计算探索了各种破碎的对称解,并将相应的能量与海森堡哈密顿量的期望值相关。尽管它们的大小在很大程度上取决于交换相关函数,但是这允许获得所有的磁耦合。有趣的是,沿着一系列研究的函数发现了磁耦合常数之间的恒定比率。当依靠自旋状态之间的能量差时,这提供了一个附加方程式,从而可以求解海森堡光谱。将由此获得的磁耦合与实验进行比较。讨论了对实验的正确解释和对更复杂系统的研究的意义。

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