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Title: Rotationally resolved pulsed field ionization photoelectron study of CO[sup +](X[sup 2][Sigma][sup +],v[sup +]=0[endash]42) in the energy range of 13. 98[endash]21. 92 eV

Journal Article · · Journal of Chemical Physics
DOI:https://doi.org/10.1063/1.480259· OSTI ID:5903350
;  [1]
  1. Ames Laboratory, USDOE and Department of Chemistry, Iowa State University Ames, Iowa 50011 (United States)

We have obtained rotationally resolved pulsed field ionization[endash]photoelectron (PFI-PE) spectra of CO in the energy range of 13.98[endash]21.92 eV, covering the ionization transitions CO[sup +](X hthinsp;[sup 2][Sigma][sup +],v[sup +]=0[endash]42,N[sup +])[l arrow]CO(X hthinsp;[sup 1][Sigma][sup +],v[sup [double prime]]=0,N[sup [double prime]]). The PFI-PE bands for CO[sup +] hthinsp;(X hthinsp;[sup 2][Sigma][sup +], v[sup +]=8[endash]22, 24, and 28[endash]39) obtained here represent the first rotationally resolved spectroscopic data for these states. The high-resolution features observed in the PFI-PE spectra allow the identification of vibrational bands for the CO[sup +] hthinsp;(X hthinsp;[sup 2][Sigma][sup +], v[sup +]=10, 14, 15, 17, 18, 21, 24, 25, 29[endash]31, 33, 35[endash]37, and 39) states, which strongly overlap with prominent vibrational bands of the CO[sup +](A hthinsp;[sup 2][Pi][sub 3/2,1/2],B hthinsp;[sup 2][Sigma][sup +]) states. The simulation using the Buckingham[endash]Orr[endash]Sichel model has provided accurate molecular constants for CO[sup +](X hthinsp;[sup 2][Sigma][sup +],v[sup +]=0[endash]42), including ionization energies, vibrational constants ([omega][sub e][sup +]=2218.8[plus minus]3.5 hthinsp;cm[sup [minus]1], [omega][sub e][sup +]x[sub e][sup +]=16.20[plus minus]0.32 hthinsp;cm[sup [minus]1], [omega][sub e][sup +]y[sub e][sup +]=0.074[plus minus]0.011 hthinsp;cm[sup [minus]1], and [omega][sub e][sup +]z[sub e][sup +]=[minus]0.001 hthinsp;83[plus minus]0.000 hthinsp;13 hthin p;cm[sup [minus]1]), and rotational constants [B[sub e][sup +]=1.9797[plus minus]0.0051 hthinsp;cm[sup [minus]1], [alpha][sub e][sup +]=0.0201[plus minus]0.0011thinspcm[sup [minus]1], [gamma][sub e][sup +]=0.000 hthinsp;122[plus minus]0.000 hthinsp;067 hthinsp;cm[sup [minus]1], z[sub e][sup +]=[minus](5.2[plus minus]1.1)[times]10[sup [minus]6] hthinsp;cm[sup [minus]1]]. Enhancement of [Delta]N[lt]0 rotational branches, attributable to field-induced rotational autoionization, was clearly discernible in PFI-PE bands for CO[sup +] hthinsp;(X hthinsp;[sup 2][Sigma][sup +], v[sup +]=0[endash]5, 11, and 12). Significant local enhancements due to near-resonance autoionization were observed for low v[sup +] ([lt]10) PFI-PE bands of CO[sup +](X hthinsp;[sup 2][Sigma][sup +]), where the density of interloper Rydberg states converging to higher ionic levels is high as manifested in the photoion spectrum. The observation of a long vibrational progression in the Franck[endash]Condon gap region, where strong autoionization states are absent, is consistent with the suggestion that high-[ital n] Rydberg states converging to highly excited vibrational levels of CO[sup +](X hthinsp;[sup 2][Sigma][sup +]) are partially populated via direct excitation to a repulsive neutral state. The relatively minor band intensity variation observed for high v[sup +] PFI-PE bands is also in accord with the direct excitation model. Since [Delta]N=0, [plus minus]1, [plus minus]2, and [plus minus]3 rotational branches are observed in the PFI-PE spectra, we conclude that the ejected photoelectrons are restricted to angular momentum continuum states l=0[endash]4. [copyright] [ital 1999 American Institute of Physics.]

OSTI ID:
5903350
Journal Information:
Journal of Chemical Physics, Vol. 111:19; ISSN 0021-9606
Country of Publication:
United States
Language:
English