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Structural-order effects in low-energy electron transmission spectra of condensed Ar, Kr, Xe, N2, CO, and O2

G. Bader

G. Perluzzo

L. G. Caron

L. Sanche

  • Départment de Physique et de Mathématiques, Université de Moncton, Moncton, New Brunswick, Canada E1A 3E9

  • Groupe C.R.M. en Sciences des Radiations, Départment de Médecine Nucléaire et de Radiobiologie, Faculté de Médecine, Université de Sherbrooke, Sherbrooke, Québec, Canada J1H 5N4

  • Centre de Recherche en Physique du Solide et Départment de Physique, Faculté des Sciences, Université de Sherbrooke, Sherbrooke, Québec, Canada J1K 2R1

  • Groupe C.R.M. en Sciences des Radiations, Départment de Médecine Nucléaire et de Radiobiologie, Faculté de Médecine, Université de Sherbrooke, Sherbrooke, Québec, Canada J1H 5N4

Phys. Rev. B 30, 78 – Published 1 July, 1984

DOI: https://doi.org/10.1103/PhysRevB.30.78

Abstract

Low-energy electron transmission spectroscopy is sensitive to crystal order and electronic band structure. The latter is responsible for minima in transmitted current whenever the incident electron energy coincides with that of a band gap. We propose a quasi-free-electron model to describe the experimental results for Ar, Kr, Xe, N2, CO, and O2 films deposited on Pt. It contains two parameters: the energy of the bottom of the conduction band V0 and an average electron effective mass m*. The onset of inelastic processes is extremely valuable in determining V0. Further knowledge of the reciprocal-lattice vectors allows a reliable fit to m* and V0. The results for Xe join smoothly to those of higher-energy low-energy electron diffraction experiments. We are also able to correlate the average atomic structure factor to the minima in the elastic mean free path of Xe.

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