Wuhan Center for Magnetic Resonance, State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan 430071, People's Republic of China.
J Chem Phys. 2012 Nov 7;137(17):174113. doi: 10.1063/1.4764358.
An eight-dimensional quantum mechanical Hamiltonian has been proposed based on Palma and Clary's model in which the non-reacting CZ(3) group keeps a C(3v) symmetry in the X + YCZ(3) ↔ XY + CZ(3) reaction J. Palma and D. C. Clary [J. Chem. Phys. 112, 1859 (2000)]. By transforming the original cartesian coordinate system (x, s) into a scaled polar coordinate system (q, γ), the vibrational Hamiltonian of CZ(3) group is expressed in a simple form with a clear physical picture. This Hamiltonian is used to investigate the H + CH(4) → H(2) + CH(3) reaction on the Jordan-Gilbert potential energy surface. The total reaction probabilities are calculated for the initial ground state, and umbrella, bending, symmetric, and asymmetric stretching excited states of CH(4) with total angular momentum J = 0. The integral cross sections for the reaction are also studied for these initial vibrational states with a centrifugal-sudden approximation. The total integral cross sections for the asymmetric stretching vibrational excited state are in good agreement with the experimental observations. The results also showed the difference of dynamical behavior between reactions from symmetric and asymmetric stretching excited states. The thermal rate constants are calculated for the temperature range T = 250-2000 K and compared with the experimental and other theoretical results.
基于 Palma 和 Clary 的模型,提出了一个八维量子力学哈密顿量,其中非反应的 CZ(3) 基团在 X + YCZ(3) ↔ XY + CZ(3) 反应 J 中保持 C(3v) 对称。J. Palma 和 D. C. Clary [J. Chem. Phys. 112, 1859 (2000)]。通过将原始笛卡尔坐标系 (x, s) 转换为缩放极坐标系 (q, γ),CZ(3) 基团的振动哈密顿量以简单的形式表示,具有清晰的物理图像。该哈密顿量用于研究 Jordan-Gilbert 势能面上的 H + CH(4) → H(2) + CH(3) 反应。对于初始基态以及 CH(4) 的伞状、弯曲、对称和不对称伸缩激发态,计算了总反应概率,总角动量 J = 0。对于这些初始振动状态,还使用离心突发近似研究了反应的积分截面。不对称伸缩振动激发态的总积分截面与实验观察结果吻合良好。结果还表明了对称和不对称伸缩激发态反应之间动力学行为的差异。计算了温度范围为 T = 250-2000 K 时的热速率常数,并与实验和其他理论结果进行了比较。