Dynamical calculations of O(3P) + OH(2Π) reaction on the CHIPR potential energy surface using the fully coupled time-dependent wave-packet approach in hyperspherical coordinates

Author(s):  
Sandip Ghosh ◽  
Rahul Sharma ◽  
Satrajit Adhikari ◽  
António J. C. Varandas

Using the rate constant obtained by fully coupled 3D time-dependent wavepacket method for forward and backward reactions, we calculate Keq(T) for the reversible process [H + O2 ⇌ O + OH] and compare with experimental measurements.

2019 ◽  
Vol 21 (36) ◽  
pp. 20166-20176 ◽  
Author(s):  
Sandip Ghosh ◽  
Rahul Sharma ◽  
Satrajit Adhikari ◽  
António J. C. Varandas

ICS calculation by time dependent wavepacket approach for H + O2 reaction using non-zero J values.


2008 ◽  
Vol 354 (1-3) ◽  
pp. 180-185 ◽  
Author(s):  
Mao-you Yang ◽  
Chuan-Lu Yang ◽  
Jian-zhong Chen ◽  
Qing-gang Zhang

2013 ◽  
Vol 12 (04) ◽  
pp. 1350030
Author(s):  
LIN-BO JI ◽  
TING-XIAN XIE ◽  
HONG-YAN WANG

The quantum time dependent wave packet (TDWP) and quasiclassical trajectory (QCT) calculations were carried out to study the exchange reaction H(2S) + H′S(2Π) → HS(2Π) + H′(2S) on the 1A′ potential energy surface (PES). The integral cross sections of the H + H′S (v = j = 0) → HS + H′ reaction calculated by the two methods were presented. The results reveal that the integral cross sections (ICS) decrease with the collision energy increasing. The result of the QCT calculations is reasonably consistent with the time-dependent wave packet. Moreover, the differential cross sections (DCS) were calculated by the QCT method at the four different collision energies, which display a forward–backward symmetry. A long-lifetime H2S intermediate complex of the exchange reaction was found according to the trajectories. In the stereodynamics investigation, the polar and dihedral angle distribution functions were calculated, which have the distinct oscillations. The oscillations could be attributed to the deep well on the 1A′ PES. However, based on the polar-angle and dihedral angle distribution functions, it could be predicted that the main product rotational angular momentum preferentially point to the positive or negative direction of y-axes.


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