Institute of Organic Chemistry, Research Centre for Natural Sciences, Hungarian Academy of Sciences, H-1525, Budapest, P.O. Box 17, Hungary.
J Phys Chem A. 2012 May 10;116(18):4445-56. doi: 10.1021/jp301243a. Epub 2012 May 2.
Quasiclassical trajectory calculations have been performed for the H + H'X(v) → X + HH' abstraction and H + H'X(v) → XH + H' (X = Cl, F) exchange reactions of the vibrationally excited diatomic reactant at a wide collision energy range extending to ultracold temperatures. Vibrational excitation of the reactant increases the abstraction cross sections significantly. If the vibrational excitation is larger than the height of the potential barrier for reaction, the reactive cross sections diverge at very low collision energies, similarly to capture reactions. The divergence is quenched by rotational excitation but returns if the reactant rotates fast. The thermal rate coefficients for vibrationally excited reactants are very large, approach or exceed the gas kinetic limit because of the capture-type divergence at low collision energies. The Arrhenius activation energies assume small negative values at and below room temperature, if the vibrational quantum number is larger than 1 for HCl and larger than 3 for HF. The exchange reaction also exhibits capture-type divergence, but the rate coefficients are larger. Comparisons are presented between classical and quantum mechanical results at low collision energies. At low collision energies the importance of the exchange reaction is enhanced by a roaming atom mechanism, namely, collisions leading to H atom exchange but bypassing the exchange barrier. Such collisions probably have a large role under ultracold conditions. The calculations indicate that for roaming to occur, long-range attractive interaction and small relative kinetic energy in the chemical reaction at the first encounter are necessary, which ensures that the partners can not leave the attractive well. Large orbital angular momentum of the primary products (equivalent to large rotational excitation in a unimolecular reaction) is favorable for roaming.
已针对振动激发的双原子反应物在广泛的碰撞能范围内(延伸至极低温)进行了 H + H'X(v) → X + HH' 缔合和 H + H'X(v) → XH + H'(X = Cl,F)交换反应的准经典轨迹计算。反应物的振动激发显著增加了缔合截面。如果振动激发大于反应的势能障碍高度,则在非常低的碰撞能下反应截面会发散,类似于捕获反应。通过转动激发可以猝灭发散,但如果反应物快速转动,则发散会恢复。对于振动激发的反应物,热速率系数非常大,接近或超过气体动力学极限,因为在低碰撞能下存在捕获型发散。如果 HCl 的振动量子数大于 1,HF 的振动量子数大于 3,则 Arrhenius 活化能在室温及以下会呈现小的负值。交换反应也表现出捕获型发散,但速率系数更大。在低碰撞能下,比较了经典和量子力学结果。在低碰撞能下,漫游原子机制增强了交换反应的重要性,即导致 H 原子交换但绕过交换势垒的碰撞。这种碰撞在极低温条件下可能具有重要作用。计算表明,为了发生漫游,在首次相遇时需要长程吸引力和化学反应中的小相对动能,这确保了反应物不能离开吸引力阱。初级产物的大轨道角动量(相当于单分子反应中的大转动激发)有利于漫游。