首页> 外文期刊>The journal of physical chemistry, A. Molecules, spectroscopy, kinetics, environment, & general theory >Photodissociation Dynamics of tert-Butyl Nitrite on Ag(111): Characterization of Translationally and Internally Excited NO Fragments
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Photodissociation Dynamics of tert-Butyl Nitrite on Ag(111): Characterization of Translationally and Internally Excited NO Fragments

机译:亚硝酸叔丁酯在Ag(111)上的光解离动力学:表征的翻译和内部激发的NO片段。

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摘要

The translational, vibrational, and rotational characteristics of nitric oxide, NO, ejected by 351 nm photodissociation of tert-butyl nitrite, (CH_3)_3CONO, adsorbed on Ag(111) have been investigated using resonance-enhanced multiphoton ionization time-of-flight (REMPI-TOF) and interpreted using a direct excitation and collisional relaxation model. There are three translational energy components denoted as collisionless, intermediate, and thermalized. The collisionless component has characteristics matching those found for gas phase monomer photolysis. The thermalized component has characteristics expected for NO accommodated to the substrate temperature, while the more complex intermediate component is qualitatively describable in terms of collisions of nascent energetic NO with surrounding species as it exists into the gas phase. There are strong v" = 1 and 2 but negligible v" = 0 contributions to the collisonless component. The collisonless component is also characterized by high rotational excitation; Gaussian rotational distributions with J_(max) = 24.5 ± 1 for v" = 1 and 29.5 ± 1 for v" = 2 provide reasonable fits. The translationally thermalized component is dominated by the v" = 0 vibrational state and by a Boltzmann rotational distribution (T_(rot) = 124 ± 30 K); i.e., all three modes of motion are thermalized. The vibrational and rotational characteristics of the intermediate translational component are more complex and will require simulation and angle-resolved REMPI for fuller elucidation.
机译:使用共振增强的多光子电离飞行时间研究了由351 nm亚硝酸叔丁酯(CH_3)_3CONO吸附在Ag(111)上351 nm光解离而产生的一氧化氮NO的平移,振动和旋转特性(REMPI-TOF),并使用直接激励和碰撞松弛模型进行解释。存在三个平移能量分量,分别表示为无碰撞,中间和热化。无碰撞组分具有与气相单体光解所发现的特征相匹配的特征。热化组分具有预期的NO适应基材温度的特性,而较复杂的中间组分在定性上可以描述为新生的高能NO与气相中存在的周围物种发生碰撞。 v“ = 1和2,但对无Collison组件的贡献可忽略不计,v” = 0。无碰撞组件的特征还在于高旋转激励。对于v“ = 1的J_(max)= 24.5±1和对于v” = 2的29.5±1的高斯旋转分布提供了合理的拟合。平移热化的分量主要由v“ = 0的振动状态和玻尔兹曼旋转分布(T_(rot)= 124±30 K)决定;即,所有三种运动模式都被热化了。中间体的振动和旋转特性平移组件更加复杂,需要进行仿真和角度解析的REMPI才能更充分地阐明。

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