کد مقاله | کد نشریه | سال انتشار | مقاله انگلیسی | نسخه تمام متن |
---|---|---|---|---|
1196060 | 964446 | 2008 | 8 صفحه PDF | دانلود رایگان |

Collision-induced photon emissions (CIE) were observed for keV CO2+·/He collisions from 190 to 1020 nm. The emissions were assigned to the Δν = 0 band of the CO2+· B 2Σu+ → X 2Πg electronic transition and the Δν = +3, +2, +1, 0, −1, −2, −3 vibrational transition progression in the CO2+· A 2Πu → X 2Πg electronic transition. The other peaks arise from the emissions of excited O· fragment atoms and the target gas. The relative intensities of the CO2+· and O· emissions are independent of the ion translational energy above 3 keV, supporting the curve-crossing mechanism for collisional excitation. Investigation of the relative intensities within the A 2Πu → X 2Πg emission of CO2+· indicates that the vibrational distribution is well described by the Franck-Condon principle at high collision energy, a consequence of short collision time but not necessarily an indication of vertical transitions. Below 3 keV ion translational energy, vibrational excitation in the A 2Πu electronic state was observed. The observation is consistent with the explanation that the reaction occurs at small impact parameters, in which short-range, repulsive interactions between the projectile and the target result in direct translational-vibrational excitation.
Graphical AbstractThe collisional excitation of CO2+ follows the curve-crossing model, even though the resulting vibrational population of the excited state looks Franck-Condon.Figure optionsDownload high-quality image (104 K)Download as PowerPoint slide
Journal: Journal of the American Society for Mass Spectrometry - Volume 19, Issue 10, October 2008, Pages 1551–1558