Differential cross sections for collisions of hexapole state-selected NO with He

The first measurements of differential inelastic collision cross sections of fully state-selected NO (j=12, Omega=12, epsilon= -1) with He are presented. Full state selection is achieved by a 2 m long hexapole, which allows for a systematic study of the effect of parity conservation and breaking on...

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Veröffentlicht in:The Journal of chemical physics 2005-12, Vol.123 (22), p.224305-224305
Hauptverfasser: Gijsbertsen, A, Linnartz, H, Rus, G, Wiskerke, A E, Stolte, S, Chandler, D W, Kłos, J
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container_end_page 224305
container_issue 22
container_start_page 224305
container_title The Journal of chemical physics
container_volume 123
creator Gijsbertsen, A
Linnartz, H
Rus, G
Wiskerke, A E
Stolte, S
Chandler, D W
Kłos, J
description The first measurements of differential inelastic collision cross sections of fully state-selected NO (j=12, Omega=12, epsilon= -1) with He are presented. Full state selection is achieved by a 2 m long hexapole, which allows for a systematic study of the effect of parity conservation and breaking on the differential cross section. The collisionally excited NO molecules are detected using a resonant (1+1') REMPI ionization scheme in combination with the velocity-mapped, ion-imaging technique. The current experimental configuration minimizes the contribution of noncolliding NO molecules in other rotational states j, Omega, epsilon--that contaminates images--and allows for study of the collision process at an unprecedented level of detail. A simple method to correct ion images for collision-induced alignment is presented as well and its performance is demonstrated. The present results show a significant difference between differential cross sections for scattering into the upper and lower component of the Lambda-doublet of NO. This result cannot be due to the energy splitting between these components.
doi_str_mv 10.1063/1.2126969
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title Differential cross sections for collisions of hexapole state-selected NO with He
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