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Breaking through the false coincidence barrier in electron-ion coincidence experiments.
Osborn, David L; Hayden, Carl C; Hemberger, Patrick; Bodi, Andras; Voronova, Krisztina; Sztáray, Bálint.
Afiliação
  • Osborn DL; Combustion Research Facility, Sandia National Laboratories, Livermore, California 94551, USA.
  • Hayden CC; Combustion Research Facility, Sandia National Laboratories, Livermore, California 94551, USA.
  • Hemberger P; Laboratory for Femtochemistry and Synchrotron Radiation, Paul Scherrer Institute, Villigen 5232, Switzerland.
  • Bodi A; Laboratory for Femtochemistry and Synchrotron Radiation, Paul Scherrer Institute, Villigen 5232, Switzerland.
  • Voronova K; Department of Chemistry, University of the Pacific, Stockton, California 95211, USA.
  • Sztáray B; Department of Chemistry, University of the Pacific, Stockton, California 95211, USA.
J Chem Phys ; 145(16): 164202, 2016 Oct 28.
Article em En | MEDLINE | ID: mdl-27802642
ABSTRACT
Photoelectron Photoion Coincidence (PEPICO) spectroscopy holds the promise of a universal, isomer-selective, and sensitive analytical technique for time-resolved quantitative analysis of bimolecular chemical reactions. Unfortunately, its low dynamic range of ∼103 has largely precluded its use for this purpose, where a dynamic range of at least 105 is generally required. This limitation is due to the false coincidence background common to all coincidence experiments, especially at high count rates. Electron/ion pairs emanating from separate ionization events but arriving within the ion time of flight (TOF) range of interest constitute the false coincidence background. Although this background has uniform intensity at every m/z value, the Poisson scatter in the false coincidence background obscures small signals. In this paper, temporal ion deflection coupled with a position-sensitive ion detector enables suppression of the false coincidence background, increasing the dynamic range in the PEPICO TOF mass spectrum by 2-3 orders of magnitude. The ions experience a time-dependent electric deflection field at a well-defined fraction of their time of flight. This deflection defines an m/z- and ionization-time dependent ion impact position for true coincidences, whereas false coincidences appear randomly outside this region and can be efficiently suppressed. When cold argon clusters are ionized, false coincidence suppression allows us to observe species up to Ar9+, whereas Ar4+ is the largest observable cluster under traditional operation. This advance provides mass-selected photoelectron spectra for fast, high sensitivity quantitative analysis of reacting systems.
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Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article
Buscar no Google
Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article