Department of Chemistry, University of Illinois at Urbana-Champaign, 600 South Mathews Avenue, Urbana, Illinois 61801, USA.
J Chem Phys. 2012 Nov 28;137(20):204118. doi: 10.1063/1.4767776.
A procedure to determine optimal vibrational coordinates is developed on the basis of an earlier idea of Thompson and Truhlar [J. Chem. Phys. 77, 3031 (1982)]. For a given molecule, these coordinates are defined as the unitary transform of the normal coordinates that minimizes the energy of the vibrational self-consistent-field (VSCF) method for the ground state. They are justified by the fact that VSCF in these coordinates becomes exact in two limiting cases: harmonic oscillators, where the optimized coordinates are normal, and noninteracting anharmonic oscillators, in which the optimized coordinates are localized on individual oscillators. A robust and general optimization algorithm is developed, which decomposes the transformation matrix into a product of Jacobi matrices, determines the rotation angle of each Jacobi matrix that minimizes the energy, and iterates the process until a minimum in the whole high dimension is reached. It is shown that the optimized coordinates are neither entirely localized nor entirely delocalized (or normal) in any of the molecules (the water, water dimer, and ethylene molecules) examined (apart from the aforementioned limiting cases). Rather, high-frequency stretching modes tend to be localized, whereas low-frequency skeletal vibrations remain normal. On the basis of these coordinates, we introduce two new vibrational structure methods: optimized-coordinate VSCF (oc-VSCF) and optimized-coordinate vibrational configuration interaction (oc-VCI). For the modes that become localized, oc-VSCF is found to outperform VSCF, whereas, for both classes of modes, oc-VCI exhibits much more rapid convergence than VCI with respect to the rank of excitations. We propose a rational configuration selection for oc-VCI when the optimized coordinates are localized. The use of the optimized coordinates in VCI with this configuration selection scheme reduces the mean absolute errors in the frequencies of the fundamentals and the first overtones/combination tones from 104.7 (VCI) to 10.7 (oc-VCI) and from 132.4 (VCI) to 8.2 (oc-VCI) cm(-1) for the water molecule and the water dimer, respectively. It is also shown that the degree of coupling in the potential for ethylene is reduced effectively from four modes to three modes by the transformation from the normal to optimized coordinates, which enhances the accuracy of oc-VCI with low-rank excitations.
基于汤普森和特鲁哈尔(J. Chem. Phys. 77, 3031 (1982))的早期想法,开发了一种确定最优振动坐标的方法。对于给定的分子,这些坐标被定义为使基态振动自洽场(VSCF)方法的能量最小化的正则坐标的幺正变换。这些坐标是合理的,因为在两种极限情况下,VSCF 在这些坐标中变得精确:谐振子,其中优化坐标是正则的,以及非相互作用的非谐振子,其中优化坐标位于单个谐振子上。开发了一种强大而通用的优化算法,该算法将变换矩阵分解为雅可比矩阵的乘积,确定每个雅可比矩阵的旋转角度,该角度使能量最小化,并迭代该过程,直到达到整个高维的最小值。结果表明,在所研究的分子(水、水二聚体和乙烯分子)中,优化坐标既不完全局部化也不完全离域(或正则)(除了上述极限情况)。相反,高频伸缩模式趋于局部化,而低频骨架振动仍然保持正则。基于这些坐标,我们引入了两种新的振动结构方法:优化坐标 VSCF(oc-VSCF)和优化坐标振动组态相互作用(oc-VCI)。对于局部化的模式,发现 oc-VSCF 优于 VSCF,而对于这两类模式,oc-VCI 相对于激发的秩表现出比 VCI 更快的收敛性。我们提出了一种合理的 oc-VCI 配置选择,当优化坐标局部化时。在 VCI 中使用这种配置选择方案,将水分子和水二聚体的基频和第一泛音/组合频的平均绝对误差从 104.7(VCI)降低到 10.7(oc-VCI)和从 132.4(VCI)降低到 8.2(oc-VCI)cm-1。还表明,通过从正则坐标到优化坐标的变换,有效地将乙烯的势中的耦合度从四个模式降低到三个模式,从而提高了低秩激发的 oc-VCI 的准确性。