Published April 15, 2009 | Version v1
Journal article

On the origin of aluminum-related cathodoluminescence emissions from sublimation grown 4H-SiC(112-bar 0)

  • 1. Department of Materials Science and Engineering, North Carolina State University, Raleigh, NC 27695 (United States)
  • 2. Maxion Technologies, Hyattsville, MD 20782 (United States)
  • 3. Analytical Instrumentation Facility, North Carolina State University, Raleigh, NC 27695 (United States)
  • 4. Department of Material Science and Engineering, Carnegie Mellon University, Pittsburgh, PA 15213-3890 (United States)

Description

The spatial origins of emissions from homoepitaxial 4H-SiC(112-bar 0) films have been investigated by cathodoluminescence, secondary ion mass spectrometry, and electron trajectory simulations. At 15 keV (300 K), the spectrum contained three peaks. The most intense peak corresponded (3.18 eV) to the nitrogen donor-to-valence band transition. The lesser two peaks at 2.94 eV and 2.75 eV involved aluminum and oxygen impurities, respectively; both impurities were determined to be in high concentrations in the film-substrate interfacial region. At 25 keV (300 K) the primary emission broadened into a band at ∼3.10 eV. Deconvolution revealed three peaks; the most intense emission was again the nitrogen donor-to-valence band transition. The remaining two peaks at 3.02 eV and 2.90 eV were consistent with transitions involving aluminum impurities. The former peak was not observed in the spectra obtained at lower electron beam energies and was correlated with the conduction band-to-aluminum acceptor level transition. Monte-Carlo simulations showed the origin of the 25 keV (300 K) spectrum was the film-substrate interface. An analysis of the aluminum impurity concentration in this region revealed that the cause of the 3.02 eV emission was a dramatic increase in the concentration of aluminum (3 x 1016 cm-3 to 1 x 1018 cm-3). The emissions comprising the 3.10 eV band were further investigated at 6 K and 25 keV. The difference in the intensity of the conduction band-to-aluminum acceptor level transition at 6 K and 300 K was attributed to thermal impurity ionization and the spike in the interfacial aluminum concentration previously described.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.apsusc.2009.02.036

Additional details

Identifiers

DOI
10.1016/j.apsusc.2009.02.036;
PII
S0169-4332(09)00188-3;

Publishing Information

Journal Title
Applied Surface Science
Journal Volume
255
Journal Issue
13-14
Journal Page Range
p. 6535-6539
ISSN
0169-4332
CODEN
ASUSEE

Optional Information

Copyright
Copyright (c) 2009 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.