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铁硫簇的自旋对称结构与振动频率

Spin-symmetrised structures and vibrational frequencies of iron-sulfur clusters.

作者信息

Cappelluti Francesco, Bencivenni Luigi, Guidoni Leonardo

机构信息

University of L'Aquila - Department of Engineering, Information Science and Mathematics, via Vetoio (Coppito), L'Aquila, Italy.

出版信息

Phys Chem Chem Phys. 2020 Aug 7;22(29):16655-16664. doi: 10.1039/d0cp01591a. Epub 2020 Jul 15.

DOI:10.1039/d0cp01591a
PMID:32667376
Abstract

Calculations of relaxed geometries of multi-centre transition metal compounds are routinely carried out using Broken Symmetry Density Functional Theory. The resulting low-spin open shell electronic state is described by one single Slater determinant and is affected by spin contamination. To alleviate this symmetry breaking, the Extended Broken Symmetry (EBS) approach can be applied to complexes with an arbitrary number of local high-spin metal ions. The actual symmetry is therefore reconstructed through minimization of an effective Hamiltonian leading to a relaxed geometry consistent with the magnetic couplings. In the present work we extend the approach already introduced by [Chu et al., J. Chem. Theory Comput., 2017, 13, 4675] to the calculation of vibrational frequencies. As prototypes we have considered the iron-sulfur clusters FeSCl and FeSCl. We have compared the results obtained for different spin states (high spin, broken symmetry and extended broken symmetry) and by using different DFT functionals (B3LYP, OPBE, BP, M06 and B2PLYP) and a post-HF method (SCS-MP2). The data have shown that for specific vibrational modes the EBS technique produces shifts up to 40 cm with respect to the routinely used Broken Symmetry approach, indicating that the use of a consistent spin-symmetrised state is a crucial ingredient for an accurate description of vibrational properties, as certified by the comparison with the experimental data for the FeSCl cluster.

摘要

多中心过渡金属化合物的松弛几何结构计算通常使用破缺对称性密度泛函理论来进行。由此产生的低自旋开壳层电子态由一个单一的斯莱特行列式描述,并且受到自旋污染的影响。为了减轻这种对称性破缺,可以将扩展破缺对称性(EBS)方法应用于具有任意数量局域高自旋金属离子的配合物。因此,通过最小化有效哈密顿量来重建实际对称性,从而得到与磁耦合相一致的松弛几何结构。在本工作中,我们将[Chu等人,《化学理论与计算杂志》,2017年,13卷,4675页]已经介绍的方法扩展到振动频率的计算。作为原型,我们考虑了铁硫簇FeSCl和FeSCl。我们比较了不同自旋态(高自旋、破缺对称性和扩展破缺对称性)以及使用不同的密度泛函理论(DFT)泛函(B3LYP、OPBE、BP、M06和B2PLYP)和一种后哈特里-福克(post-HF)方法(SCS-MP2)所获得的结果。数据表明,对于特定的振动模式,EBS技术相对于常规使用的破缺对称性方法产生的位移高达40 cm,这表明使用一致的自旋对称态是准确描述振动性质的关键因素,这一点通过与FeSCl簇的实验数据比较得到了证实。

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