Fedorov Dmitri G, Ishida Toyokazu, Kitaura Kazuo
National Institute of Advanced Science and Technology (AIST), Tsukuba, Ibaraki, Japan 305-6568.
J Phys Chem A. 2005 Mar 24;109(11):2638-46. doi: 10.1021/jp047186z.
The fragment molecular orbital method (FMO) has been generalized to allow for multilayer structure. Fragments are assigned to layers, and each layer can be described with a different basis set and/or level of electron correlation. Interlayer boundaries are treated in the general spirit of the FMO method since they also coincide with some interfragment boundaries. The question of the one- and two-layer FMO accuracy dependence upon the fragmentation scheme is also addressed. The new method has been applied to predict the reaction barrier and the reaction heat for the Diels-Alder reaction with a representative set of reactants based on dividing fragments in two layers. The 6-31G* basis set has been used for the active site and the 6-31G*, 6-31G, 3-21G, and STO-3G basis sets have been used for the substituents. Different levels of electron correlation (RHF, B3LYP, and MP2) have been applied to layers in systematic fashion. The one-layer FMO errors in the reaction barrier and the reaction heat were 2.0 kcal/mol or less for all levels applied (RHF, B3LYP, and MP2), relative to full ab initio methods. For the two-layer method the error was found to be several kcal/mol. Benchmark calculations of the activation barrier for the decarboxylation of phenylcyanoacetate by beta-cyclodextrin demonstrated that the two-layer calculations are efficient, being 36 times faster than the regular DFT, as well as accurate, with the error being 1.0 kcal/mol.
片段分子轨道方法(FMO)已被推广以适用于多层结构。片段被分配到不同的层,并且每层可以用不同的基组和/或电子相关水平来描述。层间边界按照FMO方法的一般思路处理,因为它们也与一些片段间边界重合。本文还探讨了单层和双层FMO精度对片段划分方案的依赖性问题。基于将片段划分为两层,该新方法已应用于预测具有代表性反应物集合的狄尔斯-阿尔德反应的反应势垒和反应热。活性位点使用6-31G基组,取代基使用6-31G、6-31G、3-21G和STO-3G基组。不同水平的电子相关(RHF、B3LYP和MP2)已系统地应用于各层。相对于全从头算方法,对于所有应用水平(RHF、B3LYP和MP2),单层FMO在反应势垒和反应热方面的误差为2.0千卡/摩尔或更小。对于双层方法,发现误差为几千卡/摩尔。β-环糊精催化苯甲腈乙酸酯脱羧反应活化能垒的基准计算表明,双层计算效率高,比常规DFT快36倍,并且准确,误差为1.0千卡/摩尔。