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首页> 外文期刊>The Journal of Chemical Physics >O_2(X~3∑_g~?) and O_2(a~1?g) charge exchange with simple ions
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O_2(X~3∑_g~?) and O_2(a~1?g) charge exchange with simple ions

机译:O_2(X〜3∑_g〜?)和O_2(a〜1?g)与简单离子的电荷交换

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We present theory and experiments which describe charge transfer from the X~3∑_g~- and a~1?g states of molecular oxygen and atomic and molecular cations. Included in this work are new experimental results for O_2(a~1?g) and the cations O~+, CO~+, Ar~+, and N_2~+, and new theory based on complete active space self-consistent field method calculations and an extended Langevin model to calculate rate constants for ground and excited O_2 reacting with the atomic ions Ar~+, Kr~+, Xe~+, Cl~+, and Br~+. The T-shaped orientation of the (X ? O_2)~+ potential surface is used for the calculations, including all the low lying states up to the second singlet state of the oxygen molecule b~1?_g. The calculated rate constants for both O_2(X~3∑_g~-) and O_2(a~1?g) show consistent trends with the experimental results, with a significant dependence of rate constant on charge transfer exothermicity that does not depend strongly on the nature of the cation. The comparisons with theory show that partners with exothermicities of about 1 eV have stronger interactions with O_2, leading to larger Langevin radii, and also that more of the electronic states are attractive rather than repulsive, leading to larger rate constants. Rate constants for charge transfer involving O_2(a~1?g) are similar to those for O_2(X~3∑_g~-) for a given exothermicity ignoring the electronic excitation of the O_2(a~1?g) state. This means (and the electronic structure calculations support) that the ground and excited states of O_2 have about the same attractive interactions with ions
机译:我们提供了理论和实验来描述电荷从分子氧以及原子和分子阳离子的X〜3∑_g〜-和a〜1?g状态转移。这项工作包括O_2(a〜1?g)和阳离子O〜+,CO〜+,Ar〜+和N_2〜+的新实验结果,以及基于完全有源空间自洽场方法的新理论。计算和扩展的Langevin模型,以计算地面和激发O_2与原子离子Ar〜+,Kr〜+,Xe〜+,Cl〜+和Br〜+反应的速率常数。 (X≥O_2)〜+势能面的T形取向用于计算,包括所有低位态直至氧分子b〜1≤g的第二单重态。 O_2(X〜3∑_g〜-)和O_2(a〜1?g)的速率常数与实验结果均显示出一致的趋势,速率常数对电荷转移放热的依赖性很大,而电荷转移放热的依赖性不强。阳离子的性质。与理论的比较表明,放热度大约为1 eV的伙伴与O_2的相互作用更强,从而导致较大的兰格文半径,并且更多的电子态具有吸引力而不是排斥性,从而导致更大的速率常数。忽略O_2(a〜1?g)态的电子激发,在给定的放热条件下,涉及O_2(a〜1?g)的电荷转移速率常数与O_2(X〜3∑_g〜-)的速率常数相似。这意味着(和电子结构计算支持)O_2的基态和激发态与离子具有大约相同的吸引相互作用

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