Secondary Electron Emission from Non-NEA GaAs
POSTER
Abstract
Following sub-keV electron bombardment of GaAs <100> crystals, laser-
light-induced effects in the kinetic secondary electron yield (SEY) have been
observed for p-type, n-type, and undoped samples. The SEY is measured
with super- and sub-bandgap lasers of wavelengths 812 nm and 980 nm,
respectively, coincident with the electron beam. The effects on the SEY
have been observed to vary with dopant type and laser illumination. Light-
induced effects on the secondary electron energy distribution have also been
measured. While the SEY has been measured for GaAs at higher energies (≥
1 keV) with negative electron affinity (NEA) surfaces, there are no current
studies of SEY at relatively low energies with non-NEA GaAs surfaces; with
or without laser excitation of the solid. [1,2] The work presented here is
aimed towards the development of novel sources of polarized electrons as
well as the development of new methods of time-resolved measurements of
electron emission.
[1] R. U. Martinelli et al. J. Appl. Phys., 43, 4803–4804, (2003)
[2] W. A. Gutierrez et al. Appl. Phys. Lett., 21, 249–250, (2003)
light-induced effects in the kinetic secondary electron yield (SEY) have been
observed for p-type, n-type, and undoped samples. The SEY is measured
with super- and sub-bandgap lasers of wavelengths 812 nm and 980 nm,
respectively, coincident with the electron beam. The effects on the SEY
have been observed to vary with dopant type and laser illumination. Light-
induced effects on the secondary electron energy distribution have also been
measured. While the SEY has been measured for GaAs at higher energies (≥
1 keV) with negative electron affinity (NEA) surfaces, there are no current
studies of SEY at relatively low energies with non-NEA GaAs surfaces; with
or without laser excitation of the solid. [1,2] The work presented here is
aimed towards the development of novel sources of polarized electrons as
well as the development of new methods of time-resolved measurements of
electron emission.
[1] R. U. Martinelli et al. J. Appl. Phys., 43, 4803–4804, (2003)
[2] W. A. Gutierrez et al. Appl. Phys. Lett., 21, 249–250, (2003)
Presenters
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William Truslow Newman
University of Nebraska - Lincoln
Authors
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William Truslow Newman
University of Nebraska - Lincoln
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Miranda P Bryson
University of Nebraska-Lincoln
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Ken W Trantham
Univ of Nebraska - Kearney
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Marlon Weiss
University of Nebraska - Lincoln
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Herman Batelaan
University of Nebraska - Lincoln
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Timothy J. Gay
University of Nebraska - Lincoln