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dc.creatorBiesheuvel, C. A.en_US
dc.creatorSchipper, L.en_US
dc.creatorBulthuis, J.en_US
dc.creatorJanssen, M. H. M.en_US
dc.creatorStolte, S.en_US
dc.date.accessioned2007-11-20T17:07:26Z
dc.date.available2007-11-20T17:07:26Z
dc.date.issued1995en_US
dc.identifier1995-RB-06en_US
dc.identifier.urihttp://hdl.handle.net/1811/29585
dc.descriptionAuthor Institution: Vrije Universiteit, De Boelelaan 1083. 1081 HV Amsterdam, The Netherlandsen_US
dc.description.abstract$NO_{2}$ is a small molecule which, although made up of three well-known atoms, behaves in such a manner that it is sometimes spoken of as a perverse molecule. The vibrational structure of the visible absorption spectrum of $NO_{2}$ is dominated by a strong conical intersection between the potential energy surface of the electronic ground state $\tilde{X}^{2}A_{1}$ and of the first electronically excited state $\bar{A}^{2}B_{2}$. From the study of their LIF excitation spectrum, Jost and coworkers [J. Chem. Phys. 95 (8), 5701-5718, (1991)] concluded there was "quantum" chaos in the distribution of vibronic origins in the $16000 cm^{-1}$ to $25000 cm^{-1}$ range. In our laboratory we excite a supersonically cooled beam of $NO_{2}$ molecules with a linear tunable dye laser and a Ti:Sapphire ring laser. This enables us to investigate directly the region where the vibronic chaos will start to take place $(10000 cm^{-1} to 15000 cm^{-1})$. The fluorescence is detected using a photomultiplier. In addition, we are able to detect the molecular beam using a bolometer. With this we hope to bring some order into the chaos.en_US
dc.format.extent52558 bytes
dc.format.mimetypeimage/jpeg
dc.language.isoEnglishen_US
dc.publisherOhio State Universityen_US
dc.titleStudies of $NO_{2}$ by LIF and bolometric detectionen_US
dc.typearticleen_US


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