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NO(2) 的可见和紫外光光解。

The photodissociation of NO(2) by visible and ultraviolet light.

机构信息

School of Chemistry, University of Leeds, Leeds, LS2 9JT, United Kingdom.

出版信息

Phys Chem Chem Phys. 2010 Dec 28;12(48):15766-79. doi: 10.1039/c0cp01551b. Epub 2010 Nov 16.

Abstract

We present velocity map images of the NO, O((3)P(J)) and O((1)S(0)) photofragments from NO(2) excited in the range 7.6 to 9.0 eV. The molecule was initially pumped with a visible photon between 2.82-2.95 eV (440-420 nm), below the first dissociation threshold. A second ultraviolet laser with photon energies between 4.77 and 6.05 eV (260-205 nm) was used to pump high-lying excited states of neutral NO(2) and/or probe neutral photoproducts. Analysis of the kinetic energy release spectra revealed that the NO photofragments were predominantly formed in their ground electronic state with little kinetic energy. The O((3)P(J)) and O((1)S(0)) kinetic energy distributions were also dominated by kinetically 'cold' fragments. We discuss the possible excitation schemes and conclude that the unstable photoexcited states probed in the experiment were Rydberg states coupled to dissociative valence states. We compare our results with recent time-resolved studies using similar excitation and probe photon energies.

摘要

我们呈现了在 7.6 到 9.0 eV 范围内激发的 NO_2 分子的 NO、O((3)P(J)) 和 O((1)S(0)) 光碎片的速度图图像。分子最初通过 2.82-2.95 eV(440-420nm)之间的可见光子被泵浦,低于第一离解阈值。第二个紫外激光光子能量在 4.77 和 6.05 eV(260-205nm)之间,用于泵浦中性 NO_2 的高能激发态和/或探测中性光产物。对动能释放光谱的分析表明,NO 光碎片主要以基态形成,动能较小。O((3)P(J)) 和 O((1)S(0)) 的动能分布也主要由动力学上“冷”的碎片主导。我们讨论了可能的激发方案,并得出结论,实验中探测到的不稳定光激发态是与离解价态耦合的里德伯态。我们将我们的结果与使用类似激发和探测光子能量的最近的时间分辨研究进行了比较。

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