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基态和激发振动态分子结构的准经典直接从头分子动力学。

Structures of molecules in ground and excited vibrational states from quasiclassical direct ab initio molecular dynamics.

机构信息

Center for Quantum Life Sciences and Department of Chemistry, Graduate School of Science, Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima, 739-8526 Japan.

出版信息

J Phys Chem A. 2010 Jun 3;114(21):6273-83. doi: 10.1021/jp912269v.

DOI:10.1021/jp912269v
PMID:20455585
Abstract

We demonstrate that the mean structures of molecules derived from quasiclassical direct ab initio molecular dynamics (MD) simulation, the classical simulation that takes into account quantum vibrational levels, agree well with those determined from quantum-mechanical (QM) expectation values and/or experimentally observed values. First, for a one-dimensional model potential that includes anharmonicity as the third-order potential energy term, we show that the time-averaged structure over the classical trajectory with taking account of a quantum vibrational energy level correlates with a QM structure averaged using a vibrational wave function based on the first-order perturbation theory. Next, quasiclassical direct ab initio MD and Fourier grid Hamiltonian method are applied to OH and OD radicals; the mean structures at several vibrational levels of both classical and QM methods coincide, and they are in good agreement with the structures determined experimentally. Quasiclassical direct ab initio MD is then applied to H(2)O, C(2)H(2), and C(6)H(6). For H(2)O and C(2)H(2), the classical mechanically calculated mean structural parameters agree well with the experimental values and the QM values obtained from vibrational self-consistent field. For C(2)H(2), we find that r(g)(C-H) is longer than r(e)(C-H), whereas r(mean)((0))(C-H), which is equal to r(z)(C-H), is slightly shorter than r(e)(C-H).

摘要

我们证明了源于准经典直接从头分子动力学(MD)模拟的分子的平均结构,即考虑量子振动能级的经典模拟,与从量子力学(QM)期望值和/或实验观测值确定的结构非常吻合。首先,对于包括三阶势能项的非谐一维模型势,我们表明,考虑量子振动能级的经典轨迹上的时间平均结构与基于一阶微扰理论的振动波函数的 QM 结构的平均结构相关。接下来,准经典直接从头 MD 和傅里叶网格哈密顿方法被应用于 OH 和 OD 自由基;两种方法的几个振动能级的平均结构都一致,并且与实验确定的结构非常吻合。然后,准经典直接从头 MD 被应用于 H(2)O、C(2)H(2)和 C(6)H(6)。对于 H(2)O 和 C(2)H(2),经典力学计算的平均结构参数与实验值和从振动自洽场获得的 QM 值非常吻合。对于 C(2)H(2),我们发现 r(g)(C-H)比 r(e)(C-H)长,而 r(mean)((0))(C-H),即 r(z)(C-H),比 r(e)(C-H)略短。

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