LOMC - UMR 6294, CNRS-Université du Havre, 25 Rue Philippe Lebon, BP 540, 76058 Le Havre, France.
J Chem Phys. 2013 Aug 21;139(7):074301. doi: 10.1063/1.4817933.
We present a new four dimensional potential energy surface (PES) for the CN(X(2)Σ(+))-H2 system. Both molecules were treated as rigid rotors. Potential energy was obtained from the electronic structure calculations using a partially spin-restricted coupled cluster with single, double, and perturbative triple excitations method. The four atoms were described using the augmented correlation-consistent triple zeta (aug-cc-pVTZ) basis sets augmented with mid-bond functions for improved description of van der Waals interactions. The global minimum is characterized by the well depth of 121.36 cm(-1) for the linear CN⋅⋅⋅H2 structure. The zero-order corrected dissociation energies D0 are 27.73 cm(-1) and 38.75 cm(-1) for the complex with para- and ortho-H2, respectively. These theoretical results obtained using our new PES are in excellent agreement with experimental values [Y. Chen and M. C. Heaven, J. Chem. Phys. 109, 5171 (1998)]. We perform fully quantum close coupling calculations of the rotationally inelastic cross sections of CN in collisions with para-H2 and ortho-H2 at low and intermediate energies. Corresponding rate coefficients were compared with experimental results of Brunet et al. [J. Chem. Phys. 116, 3617 (2002)]. A good agreement between theoretical and experimental results was found. Fine-structure resolved cross sections were then obtained through a recoupling technique. Significant differences exist between para- and ortho-H2 results. The propensity rules between fine-structure levels are also studied, and it is shown that the cross sections for Δj = ΔN transitions are much larger than those for Δj ≠ ΔN transitions, as expected from theoretical considerations.
我们提出了一个新的 CN(X(2)Σ(+))-H2 体系的四维势能面(PES)。两个分子都被视为刚性转子。势能是通过使用部分自旋限制的耦合簇方法,带有单、双和微扰三重激发,从电子结构计算中获得的。四个原子使用扩充相关一致的三重 zeta(aug-cc-pVTZ)基组来描述,并用中键函数进行扩充,以更好地描述范德华相互作用。线性 CN⋅⋅⋅H2 结构的全局最小值特征是 121.36 cm(-1)的深阱。对于具有对-H2 和邻-H2 的复合物,零阶校正的离解能 D0 分别为 27.73 cm(-1)和 38.75 cm(-1)。使用我们的新 PES 获得的这些理论结果与实验值[Y. Chen 和 M. C. Heaven,J. Chem. Phys. 109,5171(1998)]非常吻合。我们在低能和中能下对 CN 在与对-H2 和邻-H2 的碰撞中的转动非弹性截面进行了完全量子紧密耦合计算。相应的速率系数与 Brunet 等人的实验结果进行了比较[J. Chem. Phys. 116,3617(2002)]。理论和实验结果之间发现了很好的一致性。然后通过重新耦合法获得了精细结构分辨的截面。对-H2 和邻-H2 的结果之间存在显著差异。还研究了精细结构能级之间的倾向规则,结果表明,Δj = ΔN 跃迁的截面比Δj ≠ ΔN 跃迁的截面大得多,这与理论考虑相符。