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HOD与氩原子碰撞时的振动弛豫。

Vibrational relaxation of HOD by collisions with Ar atoms.

作者信息

Butkovskaya N I, Setser D W

机构信息

Semenov Federal Research Center of Chemical Physics, Russian Academy of Sciences, 119991 Moscow, Russian Federation.

Department of Chemistry, Kansas State University, Manhattan, Kansas 66506, USA.

出版信息

J Chem Phys. 2024 Aug 7;161(5). doi: 10.1063/5.0218695.

Abstract

Vibrational relaxation of HOD(v12, v3) molecules by collisions with Ar was studied at 298 K (v12 denotes coupled bending, v2, and OD stretching, v1, vibrational modes and v3 denotes OH stretching mode). The vibrationally excited HOD molecules were generated by exothermic abstraction reactions of OD radicals with 13 different RH reactants and observed by infrared emission from a fast-flow reactor as a function of Ar pressure and reaction time. State-specific relaxation rate constants were obtained by comparison of the time evolution of the experimental vibrational distributions with numerical kinetic calculations for vibrational populations. The relaxation mechanism was based on the relaxation scheme of H2O studied earlier with the addition of specific channels for HOD(v12, v3). Unlike H2O, energy in stretching and bending vibrations of HOD cannot be separated due to close ν1 and 2ν2 energies, which leads to fast collisional equilibration between these Fermi-resonant levels. For relaxation of the only pure bending state (10), a rate constant of (1.5 ± 0.3) × 10-13 cm3 molecule-1 s-1 was obtained. The relaxation rate of higher v12 states linearly increases with quantum number and very likely includes transfer of population from OD stretch levels, v1, to a lower energy bend level. The average rate constants for the loss of population from (01), (02), and (03) stretching states are (1.1 ± 0.3) × 10-14, (3.2 ± 1.0) × 10-14, and (5.6 ± 1.2) × 10-14 cm3 molecule-1 s-1, respectively.

摘要

在298 K下研究了HOD(v12, v3)分子与Ar碰撞时的振动弛豫(v12表示耦合弯曲振动v2和OD伸缩振动v1的组合振动模式,v3表示OH伸缩振动模式)。振动激发的HOD分子通过OD自由基与13种不同RH反应物的放热提取反应产生,并在快速流动反应器中通过红外发射作为Ar压力和反应时间的函数进行观测。通过将实验振动分布的时间演化与振动布居的数值动力学计算进行比较,获得了态特异性弛豫速率常数。弛豫机制基于早期研究的H2O弛豫方案,并增加了HOD(v12, v3)的特定通道。与H2O不同,由于ν1和2ν2能量接近,HOD的伸缩振动和弯曲振动中的能量无法分离,这导致这些费米共振能级之间的快速碰撞平衡。对于唯一的纯弯曲态(10)的弛豫,获得的速率常数为(1.5 ± 0.3) × 10-13 cm3·分子-1·s-1。较高v12态的弛豫速率随量子数线性增加,并且很可能包括布居从OD伸缩能级v1转移到较低能量的弯曲能级。从(01)、(02)和(03)伸缩态失去布居的平均速率常数分别为(1.1 ± 0.3) × 10-14、(3.2 ± 1.0) × 10-14和(5.6 ± 1.2) × 10-14 cm3·分子-1·s-1。

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