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EXPLANATION OF WHY THE RESONANT STRUCTURE SEEN IN THE (1+1) REMPI SPECTRUM OF Kr$\cdot$NO VIA THE $\tilde{A}^{2}\Sigma^{+}$ STATE APPEARS IN THE $Kr^{+}$ MASS CHANNEL AS WELL AS THE Kr$\cdot$$NO^{+}$ MASS CHANNEL

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dc.creator Bush, A. M. en_US
dc.creator Dyke, J. M. en_US
dc.creator Mack, P. en_US
dc.creator Smith, D. M. en_US
dc.creator Wright, Timothy G. en_US
dc.date.accessioned 2006-06-15T15:31:54Z
dc.date.available 2006-06-15T15:31:54Z
dc.date.issued 1996 en_US
dc.identifier 1996-RE-06 en_US
dc.identifier.uri http://hdl.handle.net/1811/13539
dc.description (a) J. C. Miller, J. Chem. Phys., 90, 4031-4036 (1989). en_US
dc.description Author Institution: Chemistry Dept., The University, Highfield, en_US
dc.description.abstract The (1+1) REMPI spectrum of the $\tilde{A}^{2}\Sigma^{+}$ state of Kr$\cdot$NO appears not only in the Kr$\cdot$$NO^{+}$ channel, as would be expected, but also in the $Kr^{+}$ channel; this is despite the fact that the ionization energy of Kr is such that three photons of the laser used would need to be absorbed in order to produce these ions. Four mechanisms are considered: Two presented previously by $Miller^{a}$ and two novel mechanisms. All the mechanisms have pros and cons, and these will be detailed in the talk. en_US
dc.format.extent 75079 bytes
dc.format.mimetype image/jpeg
dc.language.iso English en_US
dc.title EXPLANATION OF WHY THE RESONANT STRUCTURE SEEN IN THE (1+1) REMPI SPECTRUM OF Kr$\cdot$NO VIA THE $\tilde{A}^{2}\Sigma^{+}$ STATE APPEARS IN THE $Kr^{+}$ MASS CHANNEL AS WELL AS THE Kr$\cdot$$NO^{+}$ MASS CHANNEL en_US
dc.type article en_US