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arXiv 2011.06560physics.chem-ph
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用最近的密度泛函对磁化率进行基准测试

Benchmarking magnetizabilities with recent density functionals

Susi Lehtola, Maria Dimitrova, Heike Fliegl, Dage Sundholm

摘要:

我们已经评估了一组51密度泛函近似,包括最近发表的以及已经建立的泛函的磁性的准确性。准确度评估考虑了一系列的27个小分子,并基于比较预测的磁化率与文献参考值计算使用耦合簇理论与完整的单打和双打和微扰三重[CCSD(T)]采用大基组。最准确的磁化率,定义为最小的平均绝对误差,获得了BHandHLYP功能。六个研究伯克利泛函和三个范围分离佛罗里达泛函也产生准确的磁化率。一些较老的泛函,如CAM-B3 LYP、KT 1、BHLYP(BHandH)、B3 LYP和PBE 0也表现得相当好。相比之下,明尼苏达泛函的性能通常不令人满意,因此不推荐用于计算磁感应电流密度磁化率和相关的磁特性,如磁化率和核磁屏蔽。我们还表明,磁化率可以通过磁化率密度的数值积分计算,我们已经实现了这种方法作为一个新的功能,包括磁感应电流方法(GIMIC)的规范。磁化率可以计算磁感应电流密度磁化率在这种方法中,即使当磁化率作为能量的二阶导数的分析方法尚未实施。磁化率密度也可以可视化,提供在磁化率的空间原点上不容易获得的附加信息。

英文摘要:

We have assessed the accuracy for magnetic properties of a set of 51 density functional approximations, including both recently published as well as already established functionals. The accuracy assessment considers a series of 27 small molecules and is based on comparing the predicted magnetizabilities to literature reference values calculated using coupled cluster theory with full singles and doubles and perturbative triples [CCSD(T)] employing large basis sets. The most accurate magnetizabilities, defined as the smallest mean absolute error, were obtained with the BHandHLYP functional. Three of the six studied Berkeley functionals and the three range-separated Florida functionals also yield accurate magnetizabilities. Also some older functionals like CAM-B3LYP, KT1, BHLYP (BHandH), B3LYP and PBE0 perform rather well. In contrast, unsatisfactory performance was generally obtained with Minnesota functionals, which are therefore not recommended for calculations of magnetically induced current density susceptibilities, and related magnetic properties such as magnetizabilities and nuclear magnetic shieldings. We also demonstrate that magnetizabilities can be calculated by numerical integration of the magnetizability density; we have implemented this approach as a new feature in the gauge-including magnetically induced current method (GIMIC). Magnetizabilities can be calculated from magnetically induced current density susceptibilities within this approach even when analytical approaches for magnetizabilities as the second derivative of the energy have not been implemented. The magnetizability density can also be visualized, providing additional information that is not otherwise easily accessible on the spatial origin of the magnetizabilities.

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