Rotational-resolved pulsed field ionization photoelectron study of NO[sup +](X [sup 1][Sigma][sup +],v[sup +]=0[endash]32) in the energy range of 9. 24[endash]16. 80 eV
- Chemical Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720 (United States)
- Ames Laboratory, U.S. Department of Energy, Ames, Iowa 50011 (United States) Department of Chemistry, Iowa State University, Ames, Iowa 50011 (United States)
- Institute for Molecular Science, Myodaiji, Okazaki 444-8585 (Japan)
We have obtained rotationally resolved pulsed filed ionization photoelectron (PFI-PE) spectra of NO in the energy range of 9.2[endash]16.8 eV, covering ionization transitions of NO[sup +](X hthinsp;[sup 1][Sigma][sup +],v[sup +]=0[endash]32,J[sup +])[l arrow]NO(X hthinsp;[sup 2][Pi][sub 3/2,1/2],v[sup [double prime]]=0,J[sup [double prime]]). The PFI-PE bands for NO[sup +](X hthinsp;[sup 1][Sigma][sup +],v[sup +]=6[endash]32) obtained here represent the first rotationally resolved spectroscopic data for these states. The simulation using the Buckingham[endash]Orr[endash]Sichel model provides accurate molecular constants for NO[sup +](X hthinsp;[sup 1][Sigma][sup +],v[sup +]=0[endash]32), including ionization energies, vibrational constants ([omega][sub e][sup +]=2 hthinsp;382.997[plus minus]0.122 hthinsp;cm[sup [minus]1], [omega][sub e][sup +][chi][sub e][sup +]=17.437 hthinsp;84[plus minus]0.000 hthinsp;90 hthinsp;cm[sup [minus]1], [omega][sub e][sup +]y[sub e][sup +]=0.063 hthinsp;209 hthinsp;5[plus minus]3.2[times]10[sup [minus]6] hthinsp;cm[sup [minus]1], and [omega][sub e][sup +]z[sub e][sup +]=[minus]0.001 hthinsp;400 hthinsp;0[plus minus]7.2[times]10[sup [minus]8] hthinsp;cm[sup [minus]1]), and rotational constants (B[sub e][sup +]=1.996 hthinsp;608[plus minus]0.006 hthinsp;259 hthinsp;cm[sup [minus]1], [alpha][sub e][sup +]=0.020 hthinsp;103[plus minus]6.3[times]10[sup [minus]5] hthinsp;cm[sup [minus]1], and [gamma][sub e][sup +]=[minus](7.22[plus minus]2.26)[times]10[sup [minus]6] hthinsp;cm[sup [minus]1]). For v[sup +]=0[endash]15, the rotational branches are [Delta]J=J[sup +][minus]J[sup [double prime]]=[plus minus]1/2, [plus minus]3/2, [plus minus]5/2, [plus minus]7/2, and [plus minus]9/2, which correspond to the formation of photoelectron angular momentum states l=0,thinsp1, 2, and 3. The [Delta]J=[plus minus]1/2, [plus minus]3/2, [plus minus]5/2, [plus minus]7/2, [plus minus]9/2, and [plus minus]11/2 rotational branches are observed in the spectra for v[sup +]=16[endash]32, revealing the production of continuum photoelectron states l=0,thinsp1, 2, 3, and 4. The maximum [Delta]J value and intensities for high [Delta]J rotational branches are found to generally increase as v[sup +] is increased in the range of 0[endash]32. This observation is attributed to an increase in inelastic cross sections for collisions between the outgoing photoelectron and the nonspherical molecular ion core as the bond distance for NO[sup +] is increased. Thus, this observation can be taken as strong support for the electron-molecular-ion-core scattering model for angular momentum and energy exchanges in the threshold photoionization of NO. [copyright] [ital 1999 American Institute of Physics.]
- OSTI ID:
- 6325569
- Journal Information:
- Journal of Chemical Physics, Journal Name: Journal of Chemical Physics Vol. 111:7; ISSN JCPSA6; ISSN 0021-9606
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
74 ATOMIC AND MOLECULAR PHYSICS
BOND LENGTHS
CATIONS
CHALCOGENIDES
CHARGED PARTICLES
DIMENSIONS
ELECTRON SPECTROSCOPY
ENERGY LEVELS
ENERGY RANGE
EV RANGE
EV RANGE 10-100
EXCITED STATES
IONIZATION
IONIZATION POTENTIAL
IONS
LENGTH
MOLECULAR IONS
MOLECULAR STRUCTURE
NITRIC OXIDE
NITROGEN COMPOUNDS
NITROGEN OXIDES
OXIDES
OXYGEN COMPOUNDS
PHOTOELECTRON SPECTROSCOPY
PHOTOIONIZATION
ROTATIONAL STATES
SPECTROSCOPY
VIBRATIONAL STATES