Bulletin of the American Physical Society
56th Annual Meeting of the APS Division of Atomic, Molecular and Optical Physics
Monday–Friday, June 16–20, 2025; Portland, Oregon
Session H00: Poster Session II (4:00PM - 6:00PM PT)
4:00 PM,
Wednesday, June 18, 2025
Oregon Convention Center
Room: Exhibit Hall E
Abstract: H00.00020 : Secondary Electron Emission from Non-NEA GaAs*
Presenter:
William Truslow Newman
(University of Nebraska - Lincoln)
Authors:
William Truslow Newman
(University of Nebraska - Lincoln)
Miranda P Bryson
(University of Nebraska-Lincoln)
Ken W Trantham
(Univ of Nebraska - Kearney)
Marlon Weiss
(University of Nebraska - Lincoln)
Herman Batelaan
(University of Nebraska - Lincoln)
Timothy J. Gay
(University of Nebraska - Lincoln)
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)
*Work supported by NSF Awards PHY-2110358, PHY-2437820 (TJG) andPHY-2207697 (HB).
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