Imaging diffraction oscillations for inelastic collisions of NO radicals with He and D 2

We present state-to-state differential cross sections for collisions of NO molecules (X Π ,j=1/2,f) with He atoms and ortho-D (j = 0) molecules as a function of collision energy. A high angular resolution obtained using the combination of Stark deceleration and velocity map imaging allows for the ob...

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Veröffentlicht in:The Journal of chemical physics 2017-07, Vol.147 (1), p.013918
Hauptverfasser: de Jongh, Tim, Karman, Tijs, Vogels, Sjoerd N, Besemer, Matthieu, Onvlee, Jolijn, Suits, Arthur G, Thompson, James O F, Groenenboom, Gerrit C, van der Avoird, Ad, van de Meerakker, Sebastiaan Y T
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container_title The Journal of chemical physics
container_volume 147
creator de Jongh, Tim
Karman, Tijs
Vogels, Sjoerd N
Besemer, Matthieu
Onvlee, Jolijn
Suits, Arthur G
Thompson, James O F
Groenenboom, Gerrit C
van der Avoird, Ad
van de Meerakker, Sebastiaan Y T
description We present state-to-state differential cross sections for collisions of NO molecules (X Π ,j=1/2,f) with He atoms and ortho-D (j = 0) molecules as a function of collision energy. A high angular resolution obtained using the combination of Stark deceleration and velocity map imaging allows for the observation of diffraction oscillations in the angular scattering distributions. Differences in the differential cross sections and, in particular, differences in the angular spacing between individual diffraction peaks are observed. Since the masses of D and He are almost equal and since D (j = 0) may be considered as a pseudo-atom, these differences directly reflect the larger size of D as compared to He. The observations are in excellent agreement with the cross sections obtained from quantum close-coupling scattering calculations based on accurate ab initio NO-He and NO-D potential energy surfaces. For the latter, we calculated a new NO-D potential energy surface.
doi_str_mv 10.1063/1.4981023
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title Imaging diffraction oscillations for inelastic collisions of NO radicals with He and D 2
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