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关于莫勒-普列塞特临界点的性质。

On the nature of the Møller-Plesset critical point.

作者信息

Sergeev Alexey V, Goodson David Z, Wheeler Steven E, Allen Wesley D

机构信息

Department of Chemistry and Biochemistry, University of Massachusetts Dartmouth, North Dartmouth, Massachusetts 02747-2300, USA.

出版信息

J Chem Phys. 2005 Aug 8;123(6):64105. doi: 10.1063/1.1991854.

Abstract

It has been suggested [F. H. Stillinger, J. Chem. Phys. 112, 9711 (2000)] that the convergence or divergence of Møller-Plesset perturbation theory is determined by a critical point at a negative value of the perturbation parameter z at which an electron cluster dissociates from the nuclei. This conjecture is examined using configuration-interaction computations as a function of z and using a quadratic approximant analysis of the high-order perturbation series. Results are presented for the He, Ne, and Ar atoms and the hydrogen fluoride molecule. The original theoretical analysis used the true Hamiltonian without the approximation of a finite basis set. In practice, the singularity structure depends strongly on the choice of basis set. Standard basis sets cannot model dissociation to an electron cluster, but if the basis includes diffuse functions then it can model another critical point corresponding to complete dissociation of all the valence electrons. This point is farther from the origin of the z plane than is the critical point for the electron cluster, but it is still close enough to cause divergence of the perturbation series. For the hydrogen fluoride molecule a critical point is present even without diffuse functions. The basis functions centered on the H atom are far enough from the F atom to model the escape of electrons away from the fluorine end of the molecule. For the Ar atom a critical point for a one-electron ionization, which was not previously predicted, seems to be present at a positive value of the perturbation parameter. Implications of the existence of critical points for quantum-chemical applications are discussed.

摘要

有人提出[F. H. 斯蒂林格,《化学物理杂志》112, 9711 (2000)],莫勒-普莱塞特微扰理论的收敛或发散由微扰参数z取负值时的一个临界点决定,在该点电子簇从原子核解离。使用组态相互作用计算作为z的函数,并对高阶微扰级数进行二次近似分析来检验这一猜想。给出了氦、氖、氩原子以及氟化氢分子的结果。最初的理论分析使用了真实哈密顿量,没有有限基组近似。实际上,奇点结构强烈依赖于基组的选择。标准基组无法模拟到电子簇的解离,但如果基组包含弥散函数,那么它可以模拟对应于所有价电子完全解离的另一个临界点。这个点比电子簇的临界点离z平面的原点更远,但仍足够近以至于导致微扰级数发散。对于氟化氢分子,即使没有弥散函数也存在一个临界点。以氢原子为中心的基函数离氟原子足够远,能够模拟电子从分子的氟端逸出。对于氩原子,在微扰参数取正值时似乎存在一个此前未被预测到的单电子电离临界点。讨论了临界点的存在对量子化学应用的影响。

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