首页> 外文期刊>Physical chemistry chemical physics: PCCP >Dynamics of the reactions of muonium and deuterium atoms with vibrationally excited hydrogen molecules: tunneling and vibrational adiabaticity
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Dynamics of the reactions of muonium and deuterium atoms with vibrationally excited hydrogen molecules: tunneling and vibrational adiabaticity

机译:mu和氘原子与振动激发的氢分子反应的动力学:隧穿和振动绝热

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摘要

Quantum mechanical (QM) and quasiclassical trajectory (QCT) calculations have been carried out for the exchange reactions of D and Mu (Mu = muonium) with hydrogen molecules in their ground and first vibrational states. In all the cases considered, the QM rate coefficients, k(T), are in very good agreement with the available experimental results. In particular, QM calculations on the most accurate potential energy surfaces (PESs) predict a rate coefficient for the Mu + H2 (v = 1) reaction which is very close to the preliminary estimate of its experimental value at 300 K. In contrast to the D + H2 (v = 0,1) and the Mu + H2 (v = 0) reactions, the QCT calculations for Mu + H2 (v = 1) predict a much smaller k(T) than that obtained with the accurate QM method. This behaviour is indicative of tunneling. The QM reaction probabilities and total reactive cross sections show that the total energy thresholds for the reactions of Mu with H2 in v = 0 and v = 1 are very similar, whereas for the corresponding reaction with D the v = 0 total energy threshold is about 0.3 eV lower than that for v = 1. The results just mentioned can be explained by considering the vibrational adiabatic potentials along the minimum energy path. The threshold for the reaction of Mu with H2 in both v = 0 and v = 1 states is the same and is given by the height of the ground vibrational adiabatic collinear potential, whereas for the D + H2 reaction the adiabaticity is preserved and the threshold for the reaction in v = 1 is very close to the height of the v = 1 adiabatic collinear barrier. For Mu + H2 (v = 1) the reaction takes place by crossing from the v = 1 to the v = 0 adiabat, since the exit channel leading to MuH (y = 1) is not energetically accessible. At the lowest possible energies, the non-adiabatic vibrational crossing implies a strong tunneling effect through the v = 1 adiabatic barrier. Absence of tunneling in the classical calculations results in a threshold that coincides with the height of the v = 1 adiabatic barrier. Most interestingly, the expected tunneling effect in the reaction of Mu with hydrogen molecules occurs for H2 (v = 1) but not for H2 (v = 0) where zero-point-energy effects clearly dominate.
机译:D和Mu(Mu = on)与氢分子处于基态和第一振动状态的交换反应已经进行了量子力学(QM)和准经典轨迹(QCT)计算。在所有考虑的情况下,QM速率系数k(T)与可用的实验结果非常吻合。特别是,在最精确的势能面(PESs)上进行的质量管理计算可以预测Mu + H2(v = 1)反应的速率系数,该速率系数非常接近其在300 K时的实验值的初步估计值。 D + H2(v = 0,1)和Mu + H2(v = 0)反应,Mu + H2(v = 1)的QCT计算预测的k(T)比用精确QM方法获得的小得多。 。此行为表示隧穿。 QM反应概率和总反应截面表明,Mu在v = 0和v = 1时与H2反应的总能量阈值非常相似,而对于D时相应的反应,v = 0的总能量阈值约为比v = 1的情况低0.3 eV。可以通过考虑沿最小能量路径的绝热势能来解释上述结果。在v = 0和v = 1两种状态下,Mu与H2反应的阈值是相同的,并由地面振动绝热共线电位的高度给出,而对于D + H2反应,绝热性得以保留,并且该阈值v = 1中的反应非常接近v = 1绝热共线势垒的高度。对于Mu + H2(v = 1),反应是通过从v = 1到v = 0的绝热体交叉进行的,因为通向能源(MuH)的出口通道(y = 1)不易接近。在尽可能低的能量下,非绝热振动交叉意味着通过v = 1绝热势垒的强隧穿效应。经典计算中没有隧穿会导致阈值与v = 1绝热势垒的高度一致。最有趣的是,在Mu与氢分子的反应中,预期的隧穿效应发生在H2(v = 1)上,而不发生在H2(v = 0)上,其中零点能量效应明显占主导地位。

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