Vacuum emission of ballistic electrons from Au-SiO2-Si structures has been
investigated for oxide layers of various thicknesses d(ox) = 13-500 nm. In
particular for very thick layers and high field strength approximate to 5 M
V cm(-1) we measure electron energies up to 200 eV, that is 80% of the maxi
mum ballistic drive energy E-ball = eU(S). In order to enable such high-ene
rgy electrons to escape into vacuum very thin and deliberately non-perfect
Au layers (d(Au) = 8-12 nm) should be used as a top semitransparent electro
de. Obviously, no energy stabilization of emitted electrons is observed. Th
is is probably caused by defect agglomeration and the forming of defect cha
nnels. These defect channels should allow a nearly-ballistic electron trans
port until they are 'burned-out' and 'quenched-off' in a macroscopic breakd
own process. What remains is damage in the form of 'dead craters'.