Abstract

Metastable deexcitation spectroscopy was applied to study the surface valence electronic structure of clean cleaved GaAs(110). Metastable deexcitation spectroscopy was flanked by angle-resolved photoemission. An effective surface density of states was derived from the experimental spectrum through deconvolution. Two groups of states were observed in the 0--4 and 5--8 eV range of binding energy, respectively. These features were ascribed to emission from surface states. A plane-by-plane tight-binding density-of-states calculation was performed. More quantitative insights were obtained by comparing experimental and theoretical results. The most prominent feature of the first group of states of deconvolution was assigned to surface state ${\mathit{A}}_{5}$. Contributions from states ${\mathit{A}}_{4}$, ${\mathit{A}}_{3}$, ${\mathit{A}}_{1}^{\ensuremath{'}}$, and ${\mathit{A}}_{2}^{\ensuremath{'}}$ were also observed. The doublet of the second group of features was identified with ${\mathit{C}}_{2}$ and ${\mathit{C}}_{1}$. Relative amplitudes of effective surface density of states were related to surface charge density.

Highlights

  • Determination of surface and interface electronic structure is one of the main issues in modern surface physics

  • Both this value of the onset and shape clearly indicate the occurrence of a resonant ionization (RI)+Auger neutralization (AN) deexcitation process

  • It is important to stress the similarity with ion neutralization spectroscopy (INS) Auger neutralization results obtained on the same surface by Pretzer and Hagstrum (1966), using ions of 4 eV of kinetic energy

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Summary

15 DECEMBER 1995-II

Istituto Nazionale di Fisica della Materia, unita di C'enoea and Department of Physics, University of Genova, via Dodecanneso 88, 16146 Genova, Italy (Received 17 July 1995). An effective surface density of states was derived from the experimental spectrum through deconvolution. Two groups of states were observed in the 0—4 and [5,6,7,8] eV range of binding energy, respectively. These features were ascribed to emission from surface states. The most prominent feature of the first group of states of deconvolution was assigned to surface state As. Contributions from states A4, A3 A1, and A2 were observed. Relative amplitudes of effective surface density of states were related to surface charge density

INTRODUCTION
EXPERIMENT
EXPERIMENTAL RESULTS AND DISCUSSION
CONCLUSIONS
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